Optical Image Capturing System

ABSTRACT

A four-piece optical lens for capturing image and a five-piece optical module for capturing image are provided. In the order from an object side to an image side, the optical lens along the optical axis includes a first lens with positive refractive power; a second lens with refractive power; a third lens with refractive power; and a fourth lens with refractive power; and at least one of the image-side surface and object-side surface of each of the four lens elements are aspheric. The optical lens can increase aperture value and improve the imagining quality for use in compact cameras.

CROSS-REFERENCE TO RELATED APPLICATION

This application claims priority from Taiwan Patent Application No. 105123105, filed on Jul. 21, 2016, in the Taiwan Intellectual Property Office, the content of which is hereby incorporated by reference in its entirety for all purposes.

BACKGROUND OF THE INVENTION 1. Field of the Invention

The present disclosure relates to an optical image capturing system, and more particularly to a compact optical image capturing system which can be applied to electronic products.

2. Description of the Related Art

In recent years, with the rise of portable electronic devices having camera functionalities, the demand for an optical image capturing system is raised gradually. The image sensing device of ordinary photographing camera is commonly selected from charge coupled device (CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor). In addition, as advanced semiconductor manufacturing technology enables the minimization of pixel size of the image sensing device, the development of the optical image capturing system directs towards the field of high pixels. Therefore, the requirement for high imaging quality is rapidly raised.

The traditional optical image capturing system of a portable electronic device comes with different designs, including a second-lens or a third-lens design. However, the requirement for the higher pixels and the requirement for a large aperture of an end user, like functionalities of micro filming and night view, or the requirement of wide view angle of the portable electronic device have been raised. But the optical image capturing system with the large aperture design often produces more aberration, resulting in the deterioration of quality in peripheral image formation and difficulties of manufacturing, and the optical image capturing system with wide view angle design increases distortion rate in image formation, thus the optical image capturing system in prior arts cannot meet the requirement of the higher order camera lens module.

Therefore, it is a pressing issue to come up a way to effectively increase the amount of admitted light into and the angle of view of the optical image capturing system, so as to achieve a balanced design, which can minimize the size of the camera module, while meeting the users' requirement for higher total pixel count and better image quality.

SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an optical image capturing system and an optical image capturing lens, which use a combination of refractive powers, convex and concave surfaces of four-piece optical lenses (the convex or concave surface in the present disclosure denotes the geometrical shape of an image-side surface or an object-side surface of each lens on an optical axis) to increase the amount of light admitted into the optical image capturing system and the angle of view of the optical lenses. Furthermore, the lens elements of the optical image capturing system of the present invention are positioned using components with small wall thickness. As the result, the optical image capturing system of the present invention possesses a certain amount of relative illumination, the total pixel count and the image quality thereof are improved, and the present invention can be disposed in minimized or narrow bezel electronic products.

In addition, when it comes to certain application of optical imaging, there will be a need to capture image via light sources with wavelengths in both visible and infrared ranges, an example of this kind of application is IP video surveillance camera, which is equipped with the Day & Night function. The visible spectrum for human vision has wavelengths ranging from 400 to 700 nm, but the image formed on the camera sensor includes infrared light, which is invisible to human eyes. Therefore, under certain circumstances, an IR cut filter removable (ICR) is placed before the sensor of the IP video surveillance camera, in order to ensure that only the light that is visible to human eyes is picked up by the sensor eventually, so as to enhance the “fidelity” of the image. The ICR of the IP video surveillance camera can completely filter out the infrared light under daytime mode to avoid color cast; whereas under night mode, it allows infrared light to pass through the lens to enhance the image brightness. Nevertheless, the elements of the ICR occupy a significant amount of space and are expensive, which impede to the design and manufacture of miniaturized surveillance cameras in the future.

The aspect of embodiment of the present disclosure directs to an optical image capturing system and an optical image capturing lens which utilize the combination of refractive powers, convex surfaces and concave surfaces of four lens elements, as well as the selection of materials thereof, to reduce the difference between the imaging focal length of visible light and imaging focal length of infrared light, in order to achieve the near “confocal” effect without the use of ICR elements.

Various terminologies and the reference numerals thereof of the parameters of component related to the embodiments of the present invention are given below, which serve as the references for the description that follows:

Please refer to FIG. 7. The optical image capturing system may include an image sensing device (not illustrated). The image sensor may include a substrate and an image sensor. The optical image capturing system may further include a first lens positioning element 710, which is denoted by PE1. The first lens positioning element may include a base and a lens base. The lens base may be disposed with an open accommodation space and may be disposed on the substrate, such that the image sensor may be accommodated in the accommodation space. The lens base, which may be integrally formed, may be hollow and opaque. The lens base may be disposed with a barrel portion 7141 and a base portion 7142 that are interconnected. The barrel portion 7141 may have a predetermined wall thickness, which is denoted by TPE1 (thickness of the first lens positioning element 710), and a first hole 7143 and a second hole 7144 are respectively disposed at two opposite ends of the lens base. The first hole 7143 may be connected to the barrel portion 7141 and the second hole 7144 may be connected to the base portion 7142. The shortest side length of the base portion 7142, which is measured on a plane perpendicular to the optical axis, has a maximum value denoted by PhiD. The maximum inner diameter of the second hole 7144 is denoted by Phi2.

The optical image capturing system may further include a second lens positioning element 720, which is denoted by PE2. The second lens positioning element 720, which may include a positioning portion 722 and a connecting portion 724, may be accommodated in the lens base of the first lens positioning element 710. The positioning portion 722 may be hollow, and a third hole 7241 and a fourth hole 7242 may be respectively disposed at two ends of the positioning portion 722 that are opposite to each other in the direction of the optical axis. The third hole 7241 may be connected to the positioning portion 722, and the fourth hole 7242 may be connected to the base portion 7142. The third hole 7241 and the fourth hole 7242 may have a predetermined wall thickness TPE2 (thickness of the second lens positioning element 720). The positioning portion 722 may come into direct contact with any lens element of the embodiments of the present disclosure, and the positioning portion 722 is capable of accommodating the lens element and aligning the lens element on the optical axis. The connecting portion 724 may be disposed on the outer side of the positioning portion 722. The connecting portion 724 may directly couple with the barrel portion 7141 such that the second lens positioning element 720 can be accommodated in the lens base of the first lens positioning element, the optical image capturing system is capable of adjusting the focal length thereof along the optical axis, and the lens element can be positioned. The maximum outer diameter of the connecting portion 724 measured on a plane perpendicular to the optical axis is denoted by PhiC. The maximum inner diameter of the fourth hole 7242 is denoted by Phi4. The aforementioned connecting portion 724 may be disposed with screw thread, such that the second lens positioning element 720 and the lens base of the first lens positioning element 710 may be screwed together.

Any lens element in the embodiments of the present disclosure may be selectively disposed at the barrel portion 7141 of the first lens positioning element 710. Furthermore, the lens element may be nearer to the first hole 7143 than the image sensor, and the optical axis of the lens element may be perpendicular to the image sensor. Any lens element in the embodiments of the present disclosure may also be indirectly disposed in the first lens positioning element 710 through the second lens positioning element 720. Furthermore, the lens element may be nearer to the third hole 7241 than the image sensor, and the optical axis of the lens element may be perpendicular to the image sensor.

The terms and their definition for the lens element parameters in the embodiment of the present invention are shown as below for further reference.

The Lens Element Parameters Related to the Magnification of the Optical Image Capturing System

The optical image capturing system can be designed and applied to biometrics, for example, facial recognition. When the embodiment of the present disclosure is configured to capture image for facial recognition, the infrared light can be adopted as the operation wavelength. For a face of about 15 centimeters (cm) wide at a distance of 25-30 cm, at least 30 horizontal pixels can be formed in the horizontal direction of an image sensor (pixel size of 1.4 micrometers (μm)). The linear magnification of the infrared light on the image plane is LM, and it meets the following conditions: LM≧0.0003, where LM=(30 horizontal pixels)*(1.4 pixel size)/(15 cm, width of the photographed object). Alternatively, the visible light can also be adopted as the operation wavelength for image recognition. When the visible light is adopted, for a face of about 15 cm wide at a distance of 25-30 cm, at least 50 horizontal pixels can be formed in the horizontal direction of an image sensor (pixel size of 1.4 micrometers (μm)).

The Lens Element Parameter Related to a Length or a Height in the Lens Element

For visible spectrum, the present invention may adopt the wavelength of 555 nm as the primary reference wavelength and the basis for the measurement of focus shift; for infrared spectrum (700-1300 nm), the present invention may adopt the wavelength of 850 nm as the primary reference wavelength and the basis for the measurement of focus shift.

The optical image capturing system includes a first image plane and a second image plane. The first image plane is an image plane specifically for the visible light, and the first image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value at the central field of view of the first image plane; the second image plane is an image plane specifically for the infrared light, and second image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value in the central of field of view of the second image plane. The optical image capturing system also includes a first average image plane and a second average image plane. The first average image plane is an image plane specifically for the visible light, and the first average image plane is perpendicular to the optical axis. The first average image plane is installed at the average position of the defocusing positions, where the values of MTF of the visible light at the central field of view, 0.3 field of view, and the 0.7 field of view are at their respective maximum at the first spatial frequency. The second average image plane is an image plane specifically for the infrared light, and the second average image plane is perpendicular to the optical axis. The second average image plane is installed at the average position of the defocusing positions, where the values of MTF of the infrared light at the central field of view, 0.3 field of view, and the 0.7 field of view are at their respective maximum at the first spatial frequency.

The aforementioned first spatial frequency is set to be half of the spatial frequency (half frequency) of the image sensor (sensor) used in the present invention. For example, for an image sensor having the pixel size of 1.12 μm or less, the quarter spatial frequency, half spatial frequency (half frequency) and full spatial frequency (full frequency) in the characteristic diagram of modulation transfer function are at least 110 cycles/mm, 220 cycles/mm and 440 cycles/mm, respectively. Lights of any field of view can be further divided into sagittal ray and tangential ray.

The focus shifts where the through-focus MTF values of the visible sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by VSFS0, VSFS3, and VSFS7 (unit of measurement: mm), respectively. The maximum values of the through-focus MTF of the visible sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by VSMTF0, VSMTF3, and VSMTF7, respectively. The focus shifts where the through-focus MTF values of the visible tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by VTFS0, VTFS3, and VTFS7 (unit of measurement: mm), respectively. The maximum values of the through-focus MTF of the visible tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by VTMTF0, VTMTF3, and VTMTF7, respectively. The average focus shift (position) of both the aforementioned focus shifts of the visible sagittal ray at three fields of view and focus shifts of the visible tangential ray at three fields of view is denoted by AVFS (unit of measurement: mm), which equals to the absolute value |(VSFS0+VSFS3+VSFS7+VTFS0+VTFS3+VTFS7)/6|.

The focus shifts where the through-focus MTF values of the infrared sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by ISFS0, ISFS3, and ISFS7 (unit of measurement: mm), respectively. The average focus shift (position) of the aforementioned focus shifts of the infrared sagittal ray at three fields of view is denoted by AISFS (unit of measurement: mm) The maximum values of the through-focus MTF of the infrared sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by ISMTF0, ISMTF3, and ISMTF7, respectively. The focus shifts where the through-focus MTF values of the infrared tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by ITFS0, ITFS3, and ITFS7 (unit of measurement: mm), respectively. The average focus shift (position) of the aforementioned focus shifts of the infrared tangential ray at three fields of view is denoted by AITFS (unit of measurement: mm). The maximum values of the through-focus MTF of the infrared tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by ITMTF0, ITMTF3, and ITMTF7, respectively. The average focus shift (position) of both of the aforementioned focus shifts of the infrared sagittal ray at the three fields of view and focus shifts of the infrared tangential ray at the three fields of view is denoted by AIFS (unit of measurement: mm), which equals to the absolute value of |(ISFS0+ISFS3+ISFS7+ITFS0+ITFS3+ITFS7)/6|.

The focus shift (difference) between the focal points of the visible light and the infrared light at their central fields of view (RGB/IR) of the entire optical image capturing system (i.e. wavelength of 850 nm versus wavelength of 555 nm, unit of measurement: mm) is denoted by FS, which satisfies the absolute value |(VSFS0+VTFS0)/2−(ISFS0+ITFS0)/2|. The difference (focus shift) between the average focus shift of the visible light in the three fields of view and the average focus shift of the infrared light in the three fields of view (RGB/IR) of the entire optical image capturing system is denoted by AFS (i.e. wavelength of 850 nm versus wavelength of 555 nm, unit of measurement: mm), which equals to the absolute value of |AIFS−AVFS|.

The maximum height of an image formed by the optical image capturing system is denoted by HOI. The height of the optical image capturing system is denoted by HOS. A distance from the object-side surface of the first lens element to the image-side surface of the fourth lens element is denoted by InTL. A distance from the image-side surface of the fourth lens element to the first image plane is denoted by InB, where InTL+InB=HOS. A distance from an aperture stop (aperture) to the first image plane is denoted by InS. A distance from the first lens element to the second lens element is denoted by In12 (example). A central thickness of the first lens element of the optical image capturing system on the optical axis is denoted by TP1 (example).

The Lens Element Parameter Related to the Material in the Lens Element

An Abbe number of the first lens element in the optical image capturing system is denoted by NA1 (example). A refractive index of the first lens element is denoted by Nd1 (example).

The Lens Element Parameter Related to View Angle in the Lens Element

A view angle is denoted by AF. Half of the view angle is denoted by HAF. A major light angle is denoted by MRA.

The Lens Element Parameter Related to Exit/Entrance Pupil in the Lens Element

An entrance pupil diameter of the optical image capturing system is denoted by HEP. The exit pupil diameter of the optical image capturing system is the image formed with respect to the image space after the light passing through lens elements assembly behind the aperture stop. The exit pupil diameter is denoted by HXP. The maximum effective half diameter (EHD) of any surface of a single lens element refers to a perpendicular height between the optical axis and an intersection point; the intersection point is where the incident ray with the maximum view angle passes through the outermost edge of the entrance pupil, and intersects with the surface of the lens element. For example, the maximum effective half diameter of the object-side surface of the first lens element is denoted by EHD 11. The maximum effective half diameter of the image-side surface of the first lens element is denoted by EHD 12. The maximum effective half diameter of the object-side surface of the second lens element is denoted by EHD 21. The maximum effective half diameter of the image-side surface of the second lens element is denoted by EHD 22. The maximum effective half diameters of any surfaces of other lens elements in the optical image capturing system are denoted in the similar way. In the optical image capturing system of the present disclosure, the maximum effective diameter of the image-side surface of the lens element that is closest to the image plane is denoted by PhiA. The following condition is satisfied: PhiA=2 EHD. When the surface is aspheric, the terminal point of the curve defining the maximum effective diameter is the terminal point of the aspheric surface. The ineffective half diameter (IHD) of any surface of a single lens element is defined the section of the image-side surface of that lens element, in which the section extends, in a direction away from the optical axis, from the terminal point of the curve defining the maximum effective half diameter on the same surface (when the surface is aspheric, the terminal point is the point where the aspheric surface ends). In the optical image capturing system of the present disclosure, the maximum diameter of the image-side surface of the lens element that is closest to the image plane is denoted by PhiB. The following condition is satisfied: PhiB=2(EHD+IHD)=PhiA+2IHD.

In the optical image capturing system of the present disclosure, the maximum effective diameter of the image-side surface on the lens element that is closest to the image plane (i.e. image space) is the optical exit pupil thereof, and the maximum effective diameter is denoted by PhiA. For instance, when the optical exit pupil is at the image-side surface of the third lens element, the maximum effective diameter is denoted by PhiA3. When the optical exit pupil is at the image-side surface of the fourth lens element, the maximum effective diameter is denoted by PhiA4. When the optical exit pupil is at the image-side surface of the fifth lens element, the maximum effective diameter is denoted by PhiA5. When the optical exit pupil is at the image-side surface of the sixth lens element, the maximum effective diameter is denoted by PhiA6. For the optical image capturing system having different number of lens elements, the maximum effective diameter (optical exit pupil) may be denoted in similar fashion. The pupil magnification ratio of the optical image capturing system is denoted by PMR, and the following condition is satisfied: PMR=PhiA/HEP.

The Lens Element Parameter Related to the Depth of the Lens Element Shape

A distance paralleling an optical axis from a maximum effective half diameter position to an axial point on the object-side surface of the fourth lens element is denoted by InRS41 (example). A distance paralleling an optical axis from a maximum effective half diameter position to an axial point on the image-side surface of the fourth lens element is denoted by InRS42 (example).

The Lens Element Parameter Related to the Lens Element Shape

The critical point C is a point on a surface of a specific lens element, and the tangent plane to the surface at that point is perpendicular to the optical axis, wherein the point cannot be the axial point on that specific surface of the lens element. Therefore, a perpendicular distance between a critical point C31 on the object-side surface of the third lens element and the optical axis is HVT31 (example). A perpendicular distance between a critical point C32 on the image-side surface of the third lens element and the optical axis is HVT32 (example). A perpendicular distance between a critical point C41 on the object-side surface of the fourth lens element and the optical axis is HVT41 (example). A perpendicular distance between a critical point C42 on the image-side surface of the fourth lens element and the optical axis is HVT42 (example). The perpendicular distances between the critical point on the image-side surface or object-side surface of other lens elements are denoted in similar fashion.

The inflection point on object-side surface of the fourth lens element that is nearest to the optical axis is denoted by IF411, and the sinkage value of that inflection point IF411 is denoted by SGI411 (example). The sinkage value SGI411 is a horizontal distance paralleling the optical axis, which is from an axial point on the object-side surface of the fourth lens element to the inflection point nearest to the optical axis on the object-side surface of the fourth lens element. The distance perpendicular to the optical axis between the inflection point IF411 and the optical axis is HIF411 (example). The inflection point on image-side surface of the fourth lens element that is nearest to the optical axis is denoted by IF421, and the sinkage value of that inflection point IF421 is denoted by SGI421 (example). The sinkage value SGI421 is a horizontal distance paralleling the optical axis, which is from the axial point on the image-side surface of the fourth lens element to the inflection point nearest to the optical axis on the image-side surface of the fourth lens element. The distance perpendicular to the optical axis between the inflection point IF421 and the optical axis is HIF421 (example).

The object-side surface of the fourth lens element has one inflection point IF412 which is the second nearest to the optical axis and the sinkage value of the inflection point IF412 is denoted by SGI412 (example). SGI412 is a horizontal shift distance paralleling the optical axis from an axial point on the object-side surface of the fourth lens element to the inflection point which is the second nearest to the optical axis on the object-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF412 and the optical axis is HIF412 (example). The image-side surface of the fourth lens element has one inflection point IF422 which is the second nearest to the optical axis and the sinkage value of the inflection point IF422 is denoted by SGI422 (example). SGI422 is a horizontal shift distance paralleling the optical axis from an axial point on the image-side surface of the fourth lens element to the inflection point which is second nearest to the optical axis on the image-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF422 and the optical axis is HIF422 (example).

The object-side surface of the fourth lens element has one inflection point IF413 which is the third nearest to the optical axis and the sinkage value of the inflection point IF413 is denoted by SGI413 (example). SGI413 is a horizontal shift distance paralleling the optical axis from an axial point on the object-side surface of the fourth lens element to the inflection point which is the third nearest to the optical axis on the object-side surface of the fourth d lens element. A distance perpendicular to the optical axis between the inflection point IF413 and the optical axis is HIF413 (example). The image-side surface of the fourth lens element has one inflection point IF423 which is the third nearest to the optical axis and the sinkage value of the inflection point IF423 is denoted by SGI423 (example). SGI423 is a horizontal shift distance paralleling the optical axis from an axial point on the image-side surface of the fourth lens element to the inflection point which is the third nearest to the optical axis on the image-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF423 and the optical axis is HIF423 (example).

The object-side surface of the fourth lens element has one inflection point IF414 which is the fourth nearest to the optical axis and the sinkage value of the inflection point IF414 is denoted by SGI414 (example). SGI414 is a horizontal shift distance paralleling the optical axis from an axial point on the object-side surface of the fourth lens element to the inflection point which is the fourth nearest to the optical axis on the object-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF414 and the optical axis is HIF414 (example). The image-side surface of the fourth lens element has one inflection point IF424 which is the fourth nearest to the optical axis and the sinkage value of the inflection point IF424 is denoted by SGI424 (example). SGI424 is a horizontal shift distance paralleling the optical axis from an axial point on the image-side surface of the fourth lens element to the inflection point which is the fourth nearest to the optical axis on the image-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF424 and the optical axis is HIF424 (example).

The inflection points on the object-side surface or the image-side surface of the other lens elements and the perpendicular distances between them and the optical axis, or the sinkage values thereof are denoted in the similar way described above.

The Lens Element Parameter Related to the Aberration

Optical distortion for image formation in the optical image capturing system is denoted by ODT. TV distortion for image formation in the optical image capturing system is denoted by TDT. Furthermore, the degree of aberration offset within the range of 50% to 100% field of view of the formed image can be further illustrated. The offset of the spherical aberration is denoted by DFS. The offset of the coma aberration is denoted by DFC.

The purpose of the characteristic diagram of Modulation Transfer Function (MTF) of the optical image capturing system is to test and assess the contrast and sharpness of the image formed by the system. The vertical coordinate axis of the characteristic diagram of modulation transfer function represents a contrast transfer rate (values are from 0 to 1). The horizontal coordinate axis represents a spatial frequency (cycles/mm; lp/mm; line pairs per mm) Theoretically, an ideal optical image capturing system can present 100% of the line contrast of a photographed object. However, the values of the contrast transfer rate at the vertical coordinate axis are less than 1 in the actual image capturing system. In addition, comparing to the central region, it is generally more difficult to achieve fine recovery in the peripheral region of formed image. The contrast transfer rates (values of MTF) of spatial frequency of 55 cycles/mm at positions of the optical axis, 0.3 field of view and 0.7 field of view of a visible light spectrum on the first image plane are respectively denoted by MTFE0, MTFE3 and MTFE7. The contrast transfer rates (values of MTF) of spatial frequency of 110 cycles/mm at the optical axis, 0.3 field of view and 0.7 field of view on the first image plane are respectively denoted by MTFQ0, MTFQ3 and MTFQ7. The contrast transfer rates (values of MTF) of spatial frequency of 220 cycles/mm at the optical axis, 0.3 field of view and 0.7 field of view on the first image plane are respectively denoted by MTFH0, MTFH3 and MTFH7. The contrast transfer rates (values of MTF) of spatial frequency of 440 cycles/mm at the optical axis, 0.3 field of view and 0.7 field of view on the first image plane are respectively denoted by MTF0, MTF3 and MTF7. The three fields of view described above represent the center, the inner field of view and the outer field of view of the lens elements. Thus, they may be used to evaluate whether the performance of a specific optical image capturing system is excellent. The design of the optical image capturing system of the present invention mainly corresponds to a sensing device with pixel size below 1.12 micrometers inclusive. Therefore, the quarter spatial frequency, the half spatial frequency (half frequencies) and the full spatial frequency (full frequencies) of the characteristic diagram of modulation transfer function respectively are at least 110 cycles/mm, 220 cycles/mm and 440 cycles/mm.

If an optical image capturing system is to capture image with infrared spectrum, such as for the purpose of night vision in the low light condition, it might apply operation wavelength of 850 nm or 800 nm. As the main function of night vision is to recognize silhouette of an object formed in monochrome and shade, the high resolution is unnecessary, and thus, a spatial frequency, which is less than 110 cycles/mm, is used to evaluate the functionality of the optical image capturing system, when the optical image capturing system is applied to the infrared spectrum. When the foregoing wavelength of 850 nm is to be focused on the first image plane, the contrast transfer rates (values of MTF) with a spatial frequency of 55 cycles/mm at the optical axis, 0.3 field of view and 0.7 field of view on the first image plane are respectively denoted by MTFI0, MTFI3 and MTFI7. However, as the difference between infrared wavelength of 850 nm or 800 nm and that of visible light is huge, it is hard to design an optical image capturing system which is capable of focusing on the visible light and the infrared light (dual-mode) simultaneously while achieving certain performance respectively.

The disclosure provides an optical image capturing system, the object-side surface or the image-side surface of the fourth lens element may have inflection points, such that the angle of incidence from each field of view to the fourth lens element can be adjusted effectively and the optical distortion and the TV distortion can be corrected as well. Besides, the surfaces of the fourth lens element may be endowed with better capability to adjust the optical path, which yields better image quality.

An optical image capturing system is provided in accordance with the present disclosure. In the order from an object side to an image side, the optical image capturing system includes a first lens element, a second lens element, a third lens element, a fourth lens element, a first image plane, and a second image plane. The first image plane is an image plane specifically for the visible light, and the first image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value at the central field of view of the first image plane; the second image plane is an image plane specifically for the infrared light, and second image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value at the central of field of view of the second image plane. The first through fourth lens elements all have refractive powers. The focal lengths of the first lens element to the fourth lens element are f1, f2, f3, and f4 respectively. The focal length of the optical image capturing system is f. The entrance pupil diameter of the optical image capturing system is HEP. The distance on the optical axis from an object-side surface of the first lens element to the first image plane is HOS. Half of the maximum viewable angle of the optical image capturing system is denoted by HAF. The maximum image height on the first image plane perpendicular to the optical axis of the optical image capturing system is HOI. The distance on the optical axis from the object-side surface of the first lens element to the image-side surface of the fourth lens element is denoted by InTL. The maximum effective diameter of the image-side surface of the fourth lens element is denoted by PhiA4. The distance on the optical axis between the first image plane and the second image plane is denoted by FS. The thicknesses of the first to fourth lens elements at the height of ½HEP paralleling the optical axis are ETP1, ETP2, ETP3 and ETP4, respectively. The sum of ETP1 to ETP4 described above is SETP. The central thicknesses of the first to fourth lens elements on the optical axis are respectively TP1, TP2, TP3 and TP4. The sum of TP1 to TP4 described above is STP. The following conditions are satisfied: 1.2≦f/HEP≦10, 0.5≦HOS/f≦20, |FS|≦30 μm, 0<PhiA4/InTL≦2.0, and 0.5≦SETP/STP<1.

Another optical image capturing system is further provided in accordance with the present disclosure. In the order from an object side to an image side, the optical image capturing system includes a first lens element, a second lens element, a third lens element, a fourth lens element, a first image plane, a second image plane and a first lens element positioning component. The first lens positioning element may include a lens base. The lens base may be hollow and opaque. The lens base may be disposed with a barrel portion and a base portion that are interconnected. The barrel portion may be configured to accommodate the first to fourth lens elements, and the base portion may be situated between the fourth lens element and the first image plane. The base portion may have an outer perimeter that is longer than an outer perimeter of the barrel portion. The shortest side length of the base portion, which is measured on a plane perpendicular to the optical axis, has a maximum value denoted by PhiD. The first image plane is an image plane specifically for the visible light, and the first image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value at the central field of view of the first image plane; the second image plane is an image plane specifically for the infrared light, and second image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value at the central of field of view of the second image plane. The first lens element has positive refractive power. The second lens element has refractive power and has a convex image-side surface on the optical axis. The third lens element has refractive power and has a convex image-side surface on the optical axis. The focal lengths of the first lens element to the fourth lens element are f1, 12, f3, and f4 respectively. The focal length of the optical image capturing system is f. The entrance pupil diameter of the optical image capturing system is HEP. The distance on the optical axis from an object-side surface of the first lens element to the first image plane is HOS. Half of the maximum viewable angle of the optical image capturing system is denoted by HAF. The maximum image height on the first image plane perpendicular to the optical axis of the optical image capturing system is HOI. The distance on the optical axis from the object-side surface of the first lens element to the image-side surface of the fourth lens element is denoted by InTL. The maximum effective diameter of the image-side surface of the fourth lens element is denoted by PhiA4. The distance on the optical axis between the first image plane and the second image plane is denoted by FS. A horizontal distance paralleling the optical axis from a coordinate point on the object-side surface of the first lens element at the height of ½ HEP to the first image plane is ETL. A horizontal distance paralleling the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the third lens element at height of ½ HEP is EIN. The following conditions are satisfied: 1.2≦f/HEP≦10, 0.5≦HOS/f≦20, |FS|≦30 μm, 0 mm<PhiD≦5.0 mm, and 0.2≦EIN/ETL<1.

Yet another optical image capturing system is further provided in accordance with the present disclosure. In the order from an object side to an image side, the optical image capturing system includes a first lens element, a second lens element, a third lens element, a fourth lens element, a first average image plane, a second average image plane, a first lens positioning element, and a second lens positioning element. The first lens positioning element may include a lens base. The lens base may be hollow and opaque. The lens base may be disposed with a barrel portion and a base portion that are interconnected. The barrel portion may be configured to accommodate the first to fourth lens elements, and the base portion may be situated between the fourth lens element and the first average image plane. The outer perimeter of the base portion may be longer than the outer perimeter of the barrel portion. The shortest side length of the base portion, which is measured on a plane perpendicular to the optical axis, has a maximum value denoted by PhiD. The second lens positioning element may be accommodated in the lens base may include a positioning portion and a connecting portion. The positioning portion may be hollow and may come into direct contact with any lens elements to accommodate those lens elements, such that those lens elements are aligned along the optical axis. The connecting portion may be disposed at an outer side of the positioning portion and may come into direct contact with an inner perimeter of the barrel portion. The maximum outer diameter of the connecting portion, which is measured on a plane perpendicular to the optical axis, is denoted by PhiC. The first average image plane is an image plane specifically for the visible light, and the first average image plane is perpendicular to the optical axis. The first average image plane is installed at the average position of the defocusing positions, where the values of MTF of the visible light at the central field of view, 0.3 field of view, and the 0.7 field of view are at their respective maximum at the first spatial frequency. The second average image plane is an image plane specifically for the infrared light, and the second average image plane is perpendicular to the optical axis. The second average image plane is installed at the average position of the defocusing positions, where the values of MTF of the infrared light at the central field of view, 0.3 field of view, and the 0.7 field of view are at their respective maximum at the first spatial frequency. The first lens element has positive refractive power. The second lens element has refractive power and has a convex image-side surface on the optical axis. The third lens element has positive refractive power and has a convex image-side surface on the optical axis. The focal lengths of the first lens element to the fourth lens element are f1, 12, f3, and f4 respectively. The focal length of the optical image capturing system is f. The entrance pupil diameter of the optical image capturing system is HEP. The distance on the optical axis from an object-side surface of the first lens element to the first average image plane is HOS. Half of the maximum viewable angle of the optical image capturing system is denoted by HAF. The maximum image height on the first average image plane perpendicular to the optical axis of the optical image capturing system is HOI. The maximum effective diameter of the image-side surface of the fourth lens element is denoted by PhiA4. The distance between the first average image plane and the second average image plane is denoted by AFS. Half of the vertical maximum viewable angle of the optical image capturing system is denoted by VHAF. A horizontal distance paralleling the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to the first average image plane is ETL. A horizontal distance paralleling the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP is EIN. Half of the vertical maximum viewable angle of the optical image capturing system is denoted by VHAF. The following conditions are satisfied: 1.2≦f/HEP≦10, 0.5≦HOS/f≦15, 0.4≦|tan(HAF)|≦6.0, 0<PhiA4/InTL≦2.0, PhiC<PhiD, 0 mm<PhiD≦5.0 mm, 0.2≦EIN/ETL<1, |AFS|≦30 μm, and VHAF≧20 deg.

The thickness of a single lens element at height of ½ entrance pupil diameter (HEP) particularly affects the performance in correcting the optical path difference between the rays in each field of view and in correcting aberration for the shared region among the fields of view within the range of ½ entrance pupil diameter (HEP). The capability of aberration correction is enhanced when the thickness is greater, but the difficulty in manufacturing such lens also increases at the same time. Therefore, it is necessary to control the thickness of a single lens element at height of ½ entrance pupil diameter (HEP), in particular to control the proportional relation (ETP/TP) of the thickness (ETP) of the lens element at height of ½ entrance pupil diameter (HEP) to the thickness (TP) of the corresponding lens element on the optical axis. For example, the thickness of the first lens element at height of ½ entrance pupil diameter (HEP) is denoted by ETP1. The thickness of the second lens element at height of ½ entrance pupil diameter (HEP) is denoted by ETP2. The thicknesses of other lens elements are denoted in similar way. A sum of ETP1 to ETP4 described above is SETP. The embodiments of the present invention may satisfy the following condition: 0.3≦SETP/EIN≦0.8.

In order to enhance the capability of aberration correction and reduce the difficulty in manufacturing at the same time, it is particularly necessary to control the proportional relationship (ETP/TP) of the thickness (ETP) of the lens element at height of ½ entrance pupil diameter (HEP) to the thickness (TP) of the lens element on the optical axis. For example, the thickness of the first lens element at height of ½ entrance pupil diameter (HEP) is denoted by ETP1. The thickness of the first lens element on the optical axis is TP1. The ratio between both of them is ETP1/TP1. The thickness of the second lens element at height of ½ entrance pupil diameter (HEP) is denoted by ETP2. The thickness of the second lens element on the optical axis is TP2. The ratio between both of them is ETP2/TP2. The proportional relationships of the thicknesses of other lens element in the optical image capturing system at height of ½ entrance pupil diameter (HEP) to the thicknesses (TP) of the lens elements on the optical axis lens are denoted in the similar way. The embodiments of the present invention may satisfy the following condition: 0.5≦ETP/TP≦3.

A horizontal distance between two adjacent lens elements at height of ½ entrance pupil diameter (HEP) is denoted by ED. The horizontal distance (ED) described above is in parallel with the optical axis of the optical image capturing system and particularly affects the performance in correcting the optical path difference between the rays in each field of view and in correcting aberration for the shared region among the fields of view within the range of ½ entrance pupil diameter (HEP). The capability of aberration correction may be enhanced when the horizontal distance becomes greater, but the difficulty in manufacturing the lens is also increased and the degree of ‘minimization’ to the length of the optical image capturing system is restricted. Thus, it is essential to control the horizontal distance (ED) between two specific adjacent lens elements at height of ½ entrance pupil diameter (HEP).

In order to enhance the capability of aberration correction and reduce the difficulty for ‘minimization’ to the length of the optical image capturing system at the same time, it is particularly necessary to control the proportional relation (ED/IN) of the horizontal distance (ED) between the two adjacent lens elements at height of ½ entrance pupil diameter (HEP) to the horizontal distance (IN) between the two adjacent lens elements on the optical axis. For example, the horizontal distance between the first lens element and the second lens element at height of ½ entrance pupil diameter (HEP) is denoted by ED12. The horizontal distance between the first lens element and the second lens element on the optical axis is IN12. The ratio between both of them is ED12/IN12. The horizontal distance between the second lens element and the third lens element at height of ½ entrance pupil diameter (HEP) is denoted by ED23. The horizontal distance between the second lens element and the third lens element on the optical axis is IN23. The ratio between both of them is ED23/IN23. The proportional relations of the horizontal distances between other two adjacent lens elements in the optical image capturing system at height of ½ entrance pupil diameter (HEP) to the horizontal distances between the two adjacent lens elements on the optical axis are denoted in the similar way.

The horizontal distance paralleling the optical axis from a coordinate point on the image-side surface of the fourth lens element at the height of ½ HEP to the first image plane is EBL. The horizontal distance paralleling the optical axis from the axial point on the image-side surface of the fourth lens element to the first image plane is BL. In order to enhance the ability of aberration correction and reserve accommodation space for other optical elements, the embodiment of the present invention may satisfy the following conditions: 0.2≦EBL/BL≦1.1. The optical image capturing system may further include a light filtering element. The light filtering element is located between the fourth lens element and the first image plane. A distance paralleling the optical axis from a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP to the light filtering element is EIR. A distance paralleling the optical axis from an axial point on the image-side surface of the fourth lens element to the light filtering element is PIR. The embodiments of the present invention may satisfy the following condition: 0.2≦EIR/PIR≦0.8.

The optical image capturing system described above may be configured to form the image on the image sensing device which is shorter than 1/1.2 inch in diagonal length. The pixel size of the image sensing device is smaller than 1.4 micrometers (μm). Preferably the pixel size thereof is smaller than 1.12 micrometers (μm). The best pixel size thereof is smaller than 0.9 micrometers (μm). Furthermore, the optical image capturing system is applicable to the image sensing device with aspect ratio of 16:9.

The optical image capturing system described above is applicable to the demand of video recording with above millions or ten millions-pixels (e.g. 4K and 2K videos or the so-called UHD and QHD) and leads to a good imaging quality.

The height of optical system (HOS) may be reduced to achieve the minimization of the optical image capturing system when the absolute value of f1 is larger than that of f4 (|f1|>f4).

When the condition |f2|+|f3|>|f1|+|f4| is satisfied, at least one of the second through third lens elements may have weak positive refractive power or weak negative refractive power. The weak refractive power indicates that an absolute value of the focal length of a specific lens element is greater than 10. When at least one of the second through third lens elements has the weak positive refractive power, the positive refractive power of the first lens element can be shared, such that the unnecessary aberration will not appear too early. On the contrary, when at least one of the second and third lens elements has the weak negative refractive power, the aberration of the optical image capturing system can be corrected and fine-tuned.

The fourth lens element may have positive refractive power. Besides, at least one surface of the fourth lens element may possess at least one inflection point, which is capable of effectively reducing the incident angle of the off-axis rays, thereby further correcting the off-axis aberration.

BRIEF DESCRIPTION OF THE DRAWINGS

The detailed structure, operating principle and effects of the present disclosure will now be described in more details hereinafter with reference to the accompanying drawings that show various embodiments of the present disclosure as follows.

FIG. 1A is a schematic view of the optical image capturing system according to the first embodiment of the present invention.

FIG. 1B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system in the order from left to right according to the first embodiment of the present invention.

FIG. 1C is a characteristic diagram of modulation transfer of visible light spectrum for the optical image capturing system according to the first embodiment of the present invention.

FIG. 1D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the first embodiment of the present invention.

FIG. 1E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the first embodiment of the present disclosure.

FIG. 2A is a schematic view of the optical image capturing system according to the second embodiment of the present invention.

FIG. 2B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system in the order from left to right according to the second embodiment of the present invention.

FIG. 2C is a characteristic diagram of modulation transfer of visible light spectrum for the optical image capturing system according to the second embodiment of the present invention.

FIG. 2D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the second embodiment of the present invention.

FIG. 2E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the second embodiment of the present disclosure.

FIG. 3A is a schematic view of the optical image capturing system according to the third embodiment of the present invention.

FIG. 3B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system in the order from left to right according to the third embodiment of the present invention.

FIG. 3C is a characteristic diagram of modulation transfer of visible light spectrum for the optical image capturing system according to the third embodiment of the present invention.

FIG. 3D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the third embodiment of the present invention.

FIG. 3E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the third embodiment of the present disclosure.

FIG. 4A is a schematic view of the optical image capturing system according to the fourth embodiment of the present invention.

FIG. 4B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system in the order from left to right according to the fourth embodiment of the present invention.

FIG. 4C is a characteristic diagram of modulation transfer of visible light spectrum for the optical image capturing system according to the fourth embodiment of the present invention.

FIG. 4D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fourth embodiment of the present invention.

FIG. 4E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fourth embodiment of the present disclosure.

FIG. 5A is a schematic view of the optical image capturing system according to the fifth embodiment of the present invention.

FIG. 5B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system in the order from left to right according to the fifth embodiment of the present invention.

FIG. 5C is a characteristic diagram of modulation transfer of visible light spectrum for the optical image capturing system according to the fifth embodiment of the present invention.

FIG. 5D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fifth embodiment of the present invention.

FIG. 5E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fifth embodiment of the present disclosure.

FIG. 6A is a schematic view of the optical image capturing system according to the sixth embodiment of the present invention.

FIG. 6B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system in the order from left to right according to the sixth embodiment of the present invention.

FIG. 6C is a characteristic diagram of modulation transfer of visible light spectrum for the optical image capturing system according to the sixth embodiment of the present invention.

FIG. 6D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the sixth embodiment of the present invention.

FIG. 6E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the sixth embodiment of the present disclosure.

FIG. 7 is a schematic diagram illustrating the maximum effective diameter PhiA4 of the image-side surface of the fourth lens element, the maximum diameter PhiB of the image-side surface of the fourth lens element, the shortest side length PhiD of the base portion of the first lens positioning element, and the maximum outer diameter PhiC of the connecting portion of the second lens positioning element, in which PhiC and PhiD are measured on the plane perpendicular to the optical axis.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

The present invention has been described with some preferred embodiments thereof and it is understood that many changes and modifications in the described embodiments can be carried out without departing from the scope and the spirit of the invention that is intended to be limited only by the appended claims.

An optical image capturing system, in the order from an object side to an image side, includes a first, second, third and fourth lens elements with refractive powers. The optical image capturing system may further include an image sensing device, which is disposed on an image plane.

The optical image capturing system may use three sets of operation wavelengths, which are 486.1 nm, 587.5 nm and 656.2 nm, respectively, wherein 587.5 nm is served as the primary reference wavelength and a reference wavelength to obtain technical features of the optical system. The optical image capturing system may also use five sets of wavelengths which are 470 nm, 510 nm, 555 nm, 610 nm and 650 nm, respectively, wherein 555 nm is served as the primary reference wavelength and a reference wavelength to obtain technical features of the optical system.

A ratio of the focal length f of the optical image capturing system to a focal length fp of each lens element with positive refractive power is PPR. A ratio of the focal length f of the optical image capturing system to a focal length fn of each lens element with negative refractive power is NPR. A sum of the PPR of all lens elements with positive refractive powers is ΣPPR. A sum of the NPR of all lens elements with negative refractive powers is ΣNPR. The total refractive power and the total length of the optical image capturing system can be controlled easily when following conditions are satisfied: 0.5≦ΣPPR/|ΣNPR|≦4.5. Preferably, the following condition may be satisfied: 0.9≦ΣPPR/|ΣNPR|≦3.5.

The height of the optical image capturing system is HOS. When the value of the ratio, i.e. HOS/f approaches 1, it would be easier to manufacture the miniaturized optical image capturing system capable of ultra-high pixel image formation.

The sum of a focal length fp of each lens element with positive refractive power is ΣPP. A sum of a focal length fn of each lens element with negative refractive power is ΣNP. In one embodiment of the optical image capturing system of the present disclosure, the following conditions are satisfied: 0<ΣPP≦200 and f4/ΣPP≦0.85. Preferably, the following conditions may be satisfied: 0<EPP≦150 and 0.01≦f4/ΣPP≦0.7. As a result, the optical image capturing system will have better control over the focusing, and the positive refractive power of the optical system can be distributed appropriately, so as to suppress any premature formation of noticeable aberration.

The optical image capturing system may further include an image sensing device which is disposed on an image plane. Half of a diagonal of an effective detection field of the image sensing device (imaging height or the maximum image height of the optical image capturing system) is HOI. A distance on the optical axis from the object-side surface of the first lens element to the image plane is HOS. The following conditions are satisfied: HOS/HOI≦15 and 0.5≦HOS/f≦20.0. Preferably, the following conditions may be satisfied: 1≦HOS/HOI≦10 and 1≦HOS/f≦15. With this configuration, the size of the optical image capturing system can be kept small, such that a lightweight electronic product is able to accommodate it.

In addition, in the optical image capturing system of the disclosure, according to different requirements, at least one aperture stop may be arranged for reducing stray light and improving the imaging quality.

In the optical image capturing system of the disclosure, the aperture stop may be a front or middle aperture. The front aperture is the aperture stop between a photographed object and the first lens element. The middle aperture is the aperture stop between the first lens element and the image plane. If the aperture stop is the front aperture, a longer distance between the exit pupil and the image plane of the optical image capturing system can be formed, such that more optical elements can be disposed in the optical image capturing system and the efficiency of the image sensing device in receiving image can be improved. If the aperture stop is the middle aperture, the angle of view of the optical image capturing system can be expended, such that the optical image capturing system has the same advantage that is owned by wide angle cameras. A distance from the aperture stop to the image plane is InS. The following condition is satisfied: 0.2≦InS/HOS≦1.1. Preferably, the following condition may be satisfied: 0.4≦InS/HOS≦1. Hereby, the size of the optical image capturing system can be kept small without sacrificing the feature of wide angle of view.

In the optical image capturing system of the disclosure, a distance from the object-side surface of the first lens element to the image-side surface of the fourth lens element is InTL. The sum of central thicknesses of all lens elements with refractive power on the optical axis is ΣTP. The following condition is satisfied: 0.2≦ΣTP/InTL≦0.95. Preferably, the following condition may be satisfied: 0.2≦ΣTP/InTL≦0.9. Hereby, the contrast ratio for the image formation in the optical image capturing system can be improved without sacrificing the yield rate for manufacturing the lens element, and a proper back focal length is provided to accommodate other optical components in the optical image capturing system.

The curvature radius of the object-side surface of the first lens element is R1. The curvature radius of the image-side surface of the first lens element is R2. The following condition is satisfied: 0.01≦R1/R2|≦100. Preferably, the following condition may be satisfied: 0.01≦|R1/R2|≦60.

The curvature radius of the object-side surface of the fourth lens element is R9. The curvature radius of the image-side surface of the fourth lens element is R10. The following condition is satisfied: −200<(R7−R8)/(R7+R8)<30. This configuration is beneficial to the correction of the astigmatism generated by the optical image capturing system.

The distance between the first lens element and the second lens element on the optical axis is IN12. The following condition is satisfied: 0<IN12/f≦5.0. Preferably, the following condition may be satisfied: 0.01≦IN12/f≦4.0. Hereby, the chromatic aberration of the lens elements can be mitigated, such that their performance is improved.

The distance between the second lens element and the third lens element on the optical axis is IN23. The following condition is satisfied: 0<IN23/f≦5.0. Preferably, the following condition may be satisfied: 0.01≦IN23/f≦3.0. Hereby, the performance of the lens elements can be improved.

The distance between the third lens element and the fourth lens element on the optical axis is IN34. The following condition is satisfied: 0<IN34/f≦5.0. Preferably, the following condition may be satisfied: 0.001≦IN34/f≦3.0. Hereby, the performance of the lens elements can be improved.

Central thicknesses of the first lens element and the second lens element on the optical axis are TP1 and TP2, respectively. The following condition is satisfied: 1≦(TP1+IN12)/TP2≦20. Hereby, the sensitivity of the optical image capturing system can be controlled, and its performance can be improved.

Central thicknesses of the third lens element and the fourth lens element on the optical axis are TP3 and TP4, respectively, and a distance between the aforementioned two lens elements on the optical axis is IN34. The following condition is satisfied: 0.2≦(TP4+IN34)/TP4≦20. Hereby, the sensitivity produced by the optical image capturing system can be controlled and the total height of the optical image capturing system can be reduced.

The distance between the second lens element and the third lens element on the optical axis is IN23. The total sum of distances from the first lens element to the fourth lens element on the optical axis is ETP. The following condition is satisfied: 0.01≦IN23/(TP2+IN23+TP3)≦0.9. Preferably, the following condition may be satisfied: 0.05≦IN23/(TP2+IN23+TP3)≦0.7. Hereby, the aberration generated when the incident light is travelling inside the optical system can be corrected slightly layer upon layer, and the total height of the optical image capturing system can be reduced.

In the optical image capturing system of the disclosure, a distance paralleling an optical axis from a maximum effective diameter position to an axial point on the object-side surface 142 of the fourth lens element is InRS41 (InRS41 is positive if the horizontal displacement is toward the image-side surface, or InRS41 is negative if the horizontal displacement is toward the object-side surface). A distance paralleling an optical axis from a maximum effective diameter position to an axial point on the image-side surface 144 of the fourth lens element is InRS42. A central thickness of the fourth lens element 140 on the optical axis is TP4. The following conditions are satisfied: −1 mm≦InRS41≦1 mm, −1 mm≦InRS42≦1 mm, 1 mm≦|InRS41|+|InRS42|≦2 mm, 0.01≦|InRS41|/TP4≦10 and 0.01≦|InRS42|/TP4≦10. Hereby, the maximum effective diameter position between both surfaces of the fourth lens element can be controlled, so as to facilitate the aberration correction of peripheral field of view of the optical image capturing system and maintain its miniaturization effectively.

In the optical image capturing system of the disclosure, a distance paralleling an optical axis from an inflection point on the object-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI411. A distance paralleling an optical axis from an inflection point on the image-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the image-side surface of the fourth lens element is denoted by SGI421. The following conditions are satisfied: 0<SGI411/(SGI411+TP4)≦0.9 and 0<SGI421/(SGI421+TP4)≦0.9. Preferably, the following conditions may be satisfied: 0.01<SGI411/(SGI411+TP4)≦0.7 and 0.01<SGI421/(SGI421+TP4)≦0.7.

A distance paralleling the optical axis from the inflection point on the object-side surface of the fourth lens element which is the second nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI412. A distance paralleling an optical axis from an inflection point on the image-side surface of the fourth lens element which is the second nearest to the optical axis to an axial point on the image-side surface of the fourth lens element is denoted by SGI422. The following conditions are satisfied: 0<SGI412/(SGI412+TP4)≦0.9 and 0<SGI422/(SGI422+TP4)≦0.9. Preferably, the following conditions may be satisfied: 0.1≦SGI412/(SGI412+TP4)≦0.8 and 0.1≦SGI422/(SGI422+TP4)≦0.8.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is nearest to the optical axis and the optical axis is denoted by HIF411. A distance perpendicular to the optical axis between an inflection point on the image-side surface of the fourth lens element which is nearest to the optical axis and an axial point on the image-side surface of the fourth lens element is denoted by HIF421. The following conditions are satisfied: 0.01≦HIF411/HOI≦0.9 and 0.01≦HIF421/HOI≦0.9. Preferably, the following conditions may be satisfied: 0.09≦HIF411/HOI≦0.5 and 0.09≦HIF421/HOI≦0.5.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is the second nearest to the optical axis and the optical axis is denoted by HIF412. A distance perpendicular to the optical axis between an axial point on the image-side surface of the fourth lens element and an inflection point on the image-side surface of the fourth lens element which is the second nearest to the optical axis is denoted by HIF422. The following conditions are satisfied: 0.01≦HIF412/HOI≦0.9 and 0.01≦HIF422/HOI≦0.9. Preferably, the following conditions may be satisfied: 0.09≦HIF412/HOI≦0.8 and 0.09≦HIF422/HOI≦0.8.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is the third nearest to the optical axis and the optical axis is denoted by HIF413. A distance perpendicular to the optical axis between an axial point on the image-side surface of the fourth lens element and an inflection point on the image-side surface of the fourth lens element which is the third nearest to the optical axis is denoted by HIF423. The following conditions are satisfied: 0.001 mm≦|HIF413|≦5 mm and 0.001 mm≦|HIF423|≦5 mm. Preferably, the following conditions may be satisfied: 0.1 mm≦|HIF423|≦3.5 mm and 0.1 mm|HIF413|≦3.5 mm.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is the fourth nearest to the optical axis and the optical axis is denoted by HIF414. A distance perpendicular to the optical axis between an axial point on the image-side surface of the fourth lens element and an inflection point on the image-side surface of the fourth lens element which is the fourth nearest to the optical axis is denoted by HIF424. The following conditions are satisfied: 0.001 mm≦|HIF414|≦5 mm and 0.001 mm≦|HIF424|≦5 mm Preferably, the following conditions may be satisfied: 0.1 mm≦|HIF424|≦3.5 mm and 0.1 mm≦|HIF414|≦3.5 mm.

In one embodiment of the optical image capturing system of the present disclosure, the chromatic aberration of the optical image capturing system can be corrected by alternatively arranging the lens elements with large Abbe number and small Abbe number.

The equation for the aforementioned aspheric surface is:

z=ch ²/[1+[1−(k+1)c ² h ²]^(0.5) ]+A ₄ h ⁴ +A ₆ h ⁶ +A ₈ h ⁸ +A ₁₀ h ¹⁰ +A ₁₂ h ¹² +A ₁₄ h ¹⁴ ±A ₁₆ h ¹⁶ +A ₁₈ h ¹⁸ +A ₂₀ h ²⁰+ . . .  (1),

where z is a position value of the position along the optical axis and at the height h which reference to the surface apex; k is the conic coefficient, c is the reciprocal of curvature radius, and A₄, A₆, A₈, A₁₀, A₁₂, A₁₄, A₁₆, A₁₈, and A₂₀ are high order aspheric coefficients.

The optical image capturing system provided by the disclosure, the lens elements may be made of glass or plastic material. If plastic material is adopted to produce the lens elements, the cost of manufacturing as well as the weight of the lens element can be reduced effectively. If lens elements are made of glass, the heat effect can be controlled, and there will be more options to allocation the refractive powers of the lens elements in the optical image capturing system. Besides, the object-side surface and the image-side surface of the first through fourth lens elements may be aspheric, which provides more control variables, such that the number of lens elements used can be reduced in contrast to traditional glass lens element, and the aberration can be reduced too. Thus, the total height of the optical image capturing system can be reduced effectively.

In addition, in the optical image capturing system provided by the disclosure, if the lens element has a convex surface, the surface of the lens element adjacent to the optical axis is convex. If the lens element has a concave surface, the surface of the lens element adjacent to the optical axis is concave.

Besides, in the optical image capturing system of the disclosure, according to different requirements, at least one aperture stop may be arranged for reducing stray light and improving the imaging quality.

The optical image capturing system of the disclosure can be adapted to the optical image capturing system with automatic focus if required. With the features of a good aberration correction and a high quality of image formation, the optical image capturing system can be used in various applications.

The optical image capturing system of the disclosure can include a driving module according to the actual requirements. The driving module may be coupled with the lens elements and enables the movement of the lens elements. The driving module described above may be the voice coil motor (VCM) which is applied to move the lens to focus, or may be the optical image stabilization (OIS) which is applied to reduce the frequency the optical system is out of focus owing to the vibration of the lens during photo or video shooting.

At least one lens element among the first lens element, the second lens element, the third lens element and the fourth lens element of the optical image capturing system of the present disclosure may be a light filtering element which has a wavelength less than 500 nm according to the actual requirements. The light filtering element may be made by coating film on at least one surface of that lens element with certain filtering function, or forming the lens element with material that can filter light with short wavelength.

According to the above embodiments, the specific embodiments with figures are presented in detail as below.

The First Embodiment

Please refer to FIGS. 1A to 1E. FIG. 1A is a schematic view of the optical image capturing system according to the first embodiment of the present invention. FIG. 1B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system in the order from left to right according to the first embodiment of the present invention. FIG. 1C is a characteristic diagram of modulation transfer of visible light for the optical image capturing system of the first embodiment of the present invention. FIG. 1D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the first embodiment of the present invention. FIG. 1E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the first embodiment of the present disclosure. As shown in FIG. 1A, in the order from an object side to an image side, the optical image capturing system includes a first lens element 110, a second lens element 120, an aperture stop 100, a third lens element 130, a fourth lens element 140, an IR-bandstop filter 170, an image plane 180, and an image sensing device 190.

The first lens element 110 has negative refractive power and it is made of glass material. The first lens element 110 has a convex object-side surface 112 and a concave image-side surface 114, and both of the object-side surface 112 and the image-side surface 114 are aspheric. The central thickness of the first lens element on the optical axis is TP1 while the thickness of the first lens element, paralleling the optical axis, and at height of ½ entrance pupil diameter (HEP) is ETP1.

A distance paralleling an optical axis from an inflection point on the object-side surface of the first lens element which is nearest to the optical axis to an axial point on the object-side surface of the first lens element is denoted by SGI111. A distance paralleling an optical axis from an inflection point on the image-side surface of the first lens element which is nearest to the optical axis to an axial point on the image-side surface of the first lens element is denoted by SGI121. The following conditions are satisfied: SGI111=0 mm, SGI121=0 mm, |SGI111|/(|SGI111|+TP1)=0 and |SGI121|/(|SGI121|+TP1)=0.

A distance perpendicular to the optical axis from the inflection point on the object-side surface of the first lens element which is nearest to the optical axis to an axial point on the object-side surface of the first lens element is denoted by HIF111. A distance perpendicular to the optical axis from the inflection point on the image-side surface of the first lens element which is nearest to the optical axis to an axial point on the image-side surface of the first lens element is denoted by HIF121. The following conditions are satisfied: HIF111=0 mm, HIF121=0 mm, HIF111/HOI=0 and HIF121/HOI=0.

The second lens element 120 has positive refractive power and it is made of plastic material. The second lens element 120 has a concave object-side surface 122 and a convex image-side surface 124, and both of the object-side surface 122 and the image-side surface 124 are aspheric. The object-side surface 122 thereof has an inflection point. The central thickness of the second lens element on the optical axis is TP2 while the thickness paralleling the optical axis of the second lens element at the height of ½ entrance pupil diameter (HEP) is ETP2.

A distance paralleling an optical axis from an inflection point on the object-side surface of the second lens element which is nearest to the optical axis to an axial point on the object-side surface of the second lens element is denoted by SGI211. A distance paralleling an optical axis from an inflection point on the image-side surface of the second lens element which is nearest to the optical axis to an axial point on the image-side surface of the second lens element is denoted by SGI221. The following conditions are satisfied: SGI211=−0.13283 mm and SGI211|/(|SGI211|+TP2)=0.05045.

A distance perpendicular to the optical axis from the inflection point on the object-side surface of the second lens element which is nearest to the optical axis to an axial point on the object-side surface of the second lens element is denoted by HIF211. A distance perpendicular to the optical axis from the inflection point on the image-side surface of the second lens element which is nearest to the optical axis to an axial point on the image-side surface of the second lens element is denoted by HIF221. The following conditions are satisfied: HIF211=2.10379 mm and HIF211/HOI=0.69478.

The third lens element 130 has negative refractive power and it is made of plastic material. The third lens element 130 has a concave object-side surface 132 and a concave image-side surface 134, and both of the object-side surface 132 and the image-side surface 134 are aspheric. The image-side surface 134 thereof has an inflection point. The central thickness of the third lens element on the optical axis is TP3 while the thickness paralleling the optical axis of the third lens element at height of ½ entrance pupil diameter (HEP) is ETP3.

A distance paralleling an optical axis from an inflection point on the object-side surface of the third lens element which is nearest to the optical axis to an axial point on the object-side surface of the third lens element is denoted by SGI311. A distance paralleling an optical axis from an inflection point on the image-side surface of the third lens element which is nearest to the optical axis to an axial point on the image-side surface of the third lens element is denoted by SGI321. The following relationship are satisfied: SGI321=0.01218 mm, and |SGI321|/(|SGI321|+TP3)=0.03902.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens element which is nearest to the optical axis and the optical axis is denoted by HIF311. A distance perpendicular to the optical axis from the inflection point on the image-side surface of the third lens element which is nearest to the optical axis to an axial point on the image-side surface of the third lens element is denoted by HIF321. The following conditions are satisfied: HIF321=0.84373 mm and HIF321/HOI=0.27864.

The fourth lens element 140 has positive refractive power and it is made of plastic material. The fourth lens element 140 has a convex object-side surface 142 and a convex image-side surface 144; both of the object-side surface 142 and the image-side surface 144 are aspheric. The image-side surface 144 thereof has one inflection point. The central thickness of the fourth lens element on the optical axis is TP4 while the thickness paralleling the optical axis of the fourth lens element at the height of ½ entrance pupil diameter (HEP) is ETP4.

A distance paralleling an optical axis from an inflection point on the object-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI411. A distance paralleling an optical axis from an inflection point on the image-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the image-side surface of the fourth lens element is denoted by SGI421. The following conditions are satisfied: SGI411=0 mm, SGI421=−0.41627 mm, |SGI411|/(|SGI411|+TP4)=0, and |SGI421|/(|SGI421|+TP4)=0.25015.

A distance paralleling an optical axis from an inflection point on the object-side surface of the fourth lens element which is the second nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI412. The following conditions are satisfied: SGI412=0 mm and |SGI412|/(|SGI412|+TP4)=0.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is nearest to the optical axis and the optical axis is denoted by HIF411. A distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens element which is nearest to the optical axis and the optical axis is denoted by HIF421. The following conditions are satisfied: HIF411=0 mm, HIF421=1.55079 mm, HIF411/HOI=0, and HIF421/HOI=0.51215.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is second nearest to the optical axis and the optical axis is denoted by HIF412. The following conditions are satisfied: HIF412=0 mm and HIF412/HOI=0.

The horizontal distance paralleling the optical axis from a coordinate point on the object-side surface of the first lens element at the height of ½ HEP to the image plane is ETL. The horizontal distance paralleling the optical axis from a coordinate point on the object-side surface of the first lens element at the height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at the height of ½ HEP is EIN. The following conditions are satisfied: ETL=18.744 mm, EIN=12.339 mm, and EIN/ETL=0.658.

The present embodiment satisfies the following conditions: ETP1=0.949 mm, ETP2=2.483 mm, ETP3=0.345 mm, and ETP4=1.168 mm; the sum of the aforementioned values ETP1 to ETP4 is SETP, and SETP=4.945 mm. The following conditions are also satisfied: TP1=0.918 mm, TP2=2.500 mm, TP3=0.300 mm, and TP4=1.248 mm; the sum of the aforementioned values TP1 to TP4 is STP, and STP=4.966 mm, wherein SETP/STP=0.996.

In the present embodiment, the ratio (ETP/TP) of the thickness (ETP) of each lens element at the height of ½ entrance pupil diameter (HEP) to the central thickness (TP) of that lens element on the optical axis is specifically manipulated, in order to achieve a balance between the ease of manufacturing the lens elements and its capability to correct aberration. The following conditions are satisfied: ETP1/TP1=1.034, ETP2/TP2=0.993, ETP3/TP3=1.148, and ETP4/TP4=0.936.

In the present embodiment, the horizontal distance between each pair of adjacent lens elements at the height of ½ entrance pupil diameter (HEP) is manipulated as well, in order to achieve a balance among the degree of “miniaturization” for the length of the optical image capturing system HOS, the ease of manufacturing the lens elements, and its capability of aberration correction. In particular, the ratio (ED/IN) of the horizontal distance (ED) between the pair of adjacent lens elements at the height of ½ entrance pupil diameter (HEP) to the horizontal distance (IN) between the pair of adjacent lens elements on the optical axis is controlled. The following conditions are satisfied: the horizontal distance paralleling the optical axis between the first and second lens elements at the height of ½ HEP is ED12, and ED12=4.529 mm; the horizontal distance paralleling the optical axis between the second and third lens elements at the height of ½ HEP is ED23, and ED23=2.735 mm; the horizontal distance paralleling the optical axis between the third and fourth lens elements at the height of ½ HEP is ED34, and ED34=0.131 mm.

The horizontal distance between the first and second lens elements on the optical axis is denoted by IN12, where IN12=4.571 mm and ED12/IN12=0.991. The horizontal distance between the second and third lens elements on the optical axis is denoted by IN23, where IN23=2,752 mm and ED23/IN23=0.994. The horizontal distance between the third and fourth lens elements on the optical axis is denoted by IN34, where IN34=0.094 mm and ED34/IN34=1.387.

The horizontal distance paralleling the optical axis from a coordinate point on the image-side surface of the fourth lens element at the height of ½ HEP to the image plane is denoted by EBL, and EBL=6.405 mm. The horizontal distance paralleling the optical axis from the axial point on the image-side surface of the fourth lens element to the image plane is BL, and BL=6.3642 mm. The embodiment of the present invention may satisfy the following condition: EBL/BL=1.00641. In the present invention, the distance paralleling the optical axis from a coordinate point on the image-side surface of the fourth lens element at the height of ½ HEP to the IR-bandstop filter is EIR, and EIR=0.065 mm. The distance paralleling the optical axis from the axial point on the image-side surface of the fourth lens element to the IR-bandstop filter is denoted by PIR, and PIR=0.025 mm. The following condition is satisfied: EIR/PIR=2.631.

The IR-bandstop filter 170 is made of glass material and is disposed between the fourth lens element 140 and the image plane 180. The IR-bandstop filter 170 does not affect the focal length of the optical image capturing system.

In the optical image capturing system of the first embodiment, a focal length of the optical image capturing system is f, an entrance pupil diameter of the optical image capturing system is HEP, and half of a maximal view angle of the optical image capturing system is HAF. The detailed parameters are shown as below: f=2.6841 mm, f/HEP=2.7959, HAF=70 deg, and tan(HAF)=2.7475.

In the optical image capturing system of the first embodiment, a focal length of the first lens element 110 is f1 and a focal length of the fourth lens element 140 is f4. The following conditions are satisfied: f1=−5.4534 mm, |f/f1|=0.4922, f4=2.7595 mm, and |f1/f4|=1.9762.

In the optical image capturing system of the first embodiment, a focal length of the second lens element 120 is f2 and a focal length of the third lens element 130 is f3. The following conditions are satisfied: |f2|+|f3|=13.2561 mm, |f1|+|f4|=8.2129 mm, and |f2|+|f3|>|f1|+|f4|.

The ratio of the focal length f of the optical image capturing system to a focal length fp of each of lens elements with positive refractive powers is PPR. The ratio of the focal length f of the optical image capturing system to a focal length fn of each of lens elements with negative refractive powers is NPR. In the optical image capturing system of the first embodiment, a sum of the PPR of all lens elements with positive refractive powers is ΣPPR=|f/f2|+|f/f4|=1.25394. The sum of the NPR of all lens elements with negative refractive powers is ΣNPR=|f/f1|+|f/f2|=1.21490 and ΣPPR/|ΣNPR|=1.03213. The following conditions are also satisfied: |f/f1|=0.49218, |f/f2|=0.28128, |f/f3|=0.72273, and |f/f4|=0.97267.

In the optical image capturing system of the first embodiment, a distance from the object-side surface 112 of the first lens element to the image-side surface 144 of the fourth lens element is InTL. A distance from the object-side surface 112 of the first lens element to the image plane 180 is HOS. A distance from an aperture 100 to an image plane 180 is InS. Half of a diagonal length of an effective detection field of the image sensing device 190 is HOI. A distance from the image-side surface 144 of the fourth lens element to an image plane 180 is InB. The following conditions are satisfied: InTL+InB=HOS, HOS=18.74760 mm, HOI=3.088 mm, HOS/HOI=6.19141, HOS/f=6.9848, InTL/HOS=0.6605, InS=8.2310 mm, and InS/HOS=0.4390.

In the optical image capturing system of the first embodiment, the sum of central thicknesses of all lens elements with refractive power on the optical axis is ΣTP. The following conditions are satisfied: ΣTP=4.9656 mm and ΣTP/InTL=0.4010. Therefore, both contrast ratio for the image formation in the optical image capturing system and yield rate of the manufacturing process of the lens element can be balanced, and a proper back focal length is provided to accommodate other optical components in the optical image capturing system.

In the optical image capturing system of the first embodiment, a curvature radius of the object-side surface 112 of the first lens element is R1. A curvature radius of the image-side surface 114 of the first lens element is R2. The following condition is satisfied: |R1/R2|=9.6100. Hereby, the first lens element has a suitable magnitude of the positive refractive power, so as to prevent the spherical aberration from increasing too fast.

In the optical image capturing system of the first embodiment, a curvature radius of the object-side surface 142 of the fourth lens element is R7. A curvature radius of the image-side surface 144 of the fourth lens element is R8. The following condition is satisfied: (R7−R8)/(R7+R8)=−35.5932. As such, the astigmatism generated by the optical image capturing system can be corrected.

In the optical image capturing system of the first embodiment, the sum of the focal lengths for all lens elements having positive refractive power is ΣPP, which satisfies the following conditions: ΣPP=12.30183 mm, and f4/ΣPP=0.22432. Therefore, the positive refractive power of the fourth lens element 140 may be distributed to other lens elements with positive refractive power appropriately, so as to suppress noticeable aberrations generated when the incident light is propagating in the optical system.

In the optical image capturing system of the first embodiment, the sum of the focal lengths for all lens elements having negative refractive power is ΣNP, which satisfies the following conditions: ΣNP=−14.6405 mm, and f1/ΣNP=0.59488. Therefore, the negative refractive power of the first lens element 110 may be distributed to other lens elements with negative refractive power appropriately, so as to suppress noticeable aberrations generated when the incident light is propagating in the optical system.

In the optical image capturing system of the first embodiment, a distance between the first lens element 110 and the second lens element 120 on the optical axis is IN12. The following conditions are satisfied: IN12=4.5709 mm, and IN12/f=1.70299. Hereby, the chromatic aberration of the lens elements can be mitigated, such that the performance of the optical system is increased.

In the optical image capturing system of the first embodiment, a distance between the second lens element 120 and the third lens element 130 on the optical axis is IN23. The following conditions are satisfied: IN23=2.7524 mm, IN23/f=1.02548. Hereby, the chromatic aberration of the lens elements can be mitigated, such that the performance of the optical system is increased.

In the optical image capturing system of the first embodiment, a distance between the third lens element 130 and the fourth lens element 140 on the optical axis is IN34. The following conditions are satisfied: IN34=0.0944 mm and IN34/f=0.03517. Hereby, the chromatic aberration of the lens elements can be mitigated, such that the performance of the optical system is increased.

In the optical image capturing system of the first embodiment, central thicknesses of the first lens element 110 and the second lens element 120 on the optical axis are TP1 and TP2, respectively. The following conditions are satisfied: TP1=0.9179 mm, TP2=2.5000 mm, TP1/TP2=0.36715, and (TP1+IN12)/TP2=2.19552. Hereby, the sensitivity of the optical image capturing system can be controlled, and the performance thereof can be improved.

In the optical image capturing system of the first embodiment, central thicknesses of the third lens element 130 and the fourth lens element 140 on the optical axis are TP3 and TP4, respectively. The separation distance between the third lens element 130 and the fourth lens element 140 on the optical axis is IN34. The following conditions are satisfied: TP3=0.3 mm, TP4=1.2478 mm, TP3/TP4=0.24043, and (TP4+IN34)/TP3=4.47393. Hereby, the sensitivity of the optical image capturing system can be controlled, and the total height of the optical image capturing system can be reduced.

In the optical image capturing system of the first embodiment, the following conditions are satisfied: IN23/(TP2+IN23+TP3)=0.49572. Hereby, the aberration generated when the incident light is propagating inside the optical system can be corrected slightly by each lens element, and the total height of the optical image capturing system can be reduced.

In the optical image capturing system of the first embodiment, a distance paralleling an optical axis from a maximum effective diameter position to an axial point on the object-side surface 142 of the fourth lens element is InRS41. A distance paralleling an optical axis from a maximum effective diameter position to an axial point on the image-side surface 144 of the fourth lens element is InRS42. A central thickness of the fourth lens element 140 is TP4. The following conditions are satisfied: InRS41=0.2955 mm, InRS42=−0.4940 mm, |InRS41|+|InRS42|=0.7894 mm, |InRS41|/TP4=0.23679, and |InRS42|/TP4=0.39590. This configuration is favorable to the manufacturing and forming of lens elements, as well as the minimization of the optical image capturing system.

In the optical image capturing system of the first embodiment, a distance perpendicular to the optical axis between a critical point C41 on the object-side surface 142 of the fourth lens element and the optical axis is HVT41. A distance perpendicular to the optical axis between a critical point C42 on the image-side surface 144 of the fourth lens element and the optical axis is HVT42. The following conditions are satisfied: HVT41=0 mm and HVT42=0 mm.

In the optical image capturing system of the first embodiment, the following condition is satisfied: HVT42/HOI=0.

In the optical image capturing system of the first embodiment, the following condition is satisfied: HVT42/HOS=0.

In the optical image capturing system of the first embodiment, the Abbe number of the first lens element is NA1. The Abbe number of the second lens element is NA2. The Abbe number of the third lens element is NA3. The Abbe number of the fourth lens element is NA4. The following conditions are satisfied: |NA1−NA2|=0.0351. Hereby, the chromatic aberration of the optical image capturing system can be corrected.

In the optical image capturing system of the first embodiment, TV distortion and optical distortion for image formation in the optical image capturing system are TDT and ODT, respectively. The following conditions are satisfied: TDT=37.4846% and ODT=−55.3331%

In the present embodiment, the lights of any field of view can be further divided into sagittal ray and tangential ray, and the spatial frequency of 220 cycles/mm serves as the benchmark for assessing the focus shifts and the values of MTF. The focus shifts where the through-focus MTF values of the visible sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima are denoted by VSFS0, VSFS3, and VSFS7 (unit of measurement mm), respectively. The values of VSFS0, VSFS3, and VSFS7 equal to 0.00000 mm, 0.00000 mm, and 0.00000 mm, respectively. The maximum values of the through-focus MTF of the visible sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by VSMTF0, VSMTF3, and VSMTF7, respectively. The values of VSMTF0, VSMTF3, and VSMTF7 equal to 0.416, 0.397, and 0.342, respectively. The focus shifts where the through-focus MTF values of the visible tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by VTFS0, VTFS3, and VTFS7 (unit of measurement: mm), respectively. The values of VTFS0, VTFS3, and VTFS7 equal to 0.00000 mm, 0.00000 mm, and −0.01000 mm, respectively. The maximum values of the through-focus MTF of the visible tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by VTMTF0, VTMTF3, and VTMTF7, respectively. The values of VTMTF0, VTMTF3, and VTMTF7 equal to 0.416, 0.34, and 0.139, respectively. The average focus shift (position) of both the aforementioned focus shifts of the visible sagittal ray at three fields of view and focus shifts of the visible tangential ray at three fields of view is denoted by AVFS (unit of measurement: mm), which satisfies the absolute value |(VSFS0+VSFS3+VSFS7+VTFS0+VTFS3+VTFS7)/6|=|−0.00200 mm|.

The focus shifts where the through-focus MTF values of the infrared sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by ISFS0, ISFS3, and ISFS7 (unit of measurement: mm), respectively. The values of ISFS0, ISFS3, and ISFS7 equal to 0.03000 mm, 0.03300 mm, and 0.03300 mm, respectively. The average focus shift (position) of the aforementioned focus shifts of the infrared sagittal ray at three fields of view is denoted by AISFS (unit of measurement: mm) The maximum values of the through-focus MTF of the infrared sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by ISMTF0, ISMTF3, and ISMTF7, respectively. The values of ISMTF0, ISMTF3, and ISMTF7 equal to 0.169, 0.148, and 0.089, respectively. The focus shifts where the through-focus MTF values of the infrared tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by ITFS0, ITFS3, and ITFS7 (unit of measurement: mm), respectively. The values of ITFS0, ITFS3, and ITFS7 equal to 0.03, 0.028, and 0.005, respectively. The average focus shift (position) of the aforementioned focus shifts of the infrared tangential ray at three fields of view is denoted by AITFS (unit of measurement: mm) The maximum values of the through-focus MTF of the infrared tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by ITMTF0, ITMTF3, and ITMTF7, respectively. The values of ITMTF0, ITMTF3, and ITMTF7 equal to 0.169, 0.093, and 0.00000, respectively. The average focus shift (position) of both of the aforementioned focus shifts of the infrared sagittal ray at the three fields of view and focus shifts of the infrared tangential ray at the three fields of view is denoted by AIFS (unit of measurement: mm), which equals to the absolute value of |(ISFS0+ISFS3+ISFS7+ITFS0+ITFS3+ITFS7)/6|=|0.02600 mm|.

The focus shift (difference) between the focal points of the visible light and the infrared light at their central fields of view (RGB/IR) of the entire optical image capturing system (i.e. wavelength of 850 nm versus wavelength of 555 nm, unit of measurement: mm) is denoted by FS, which satisfies the absolute value |(VSFS0+VTFS0)/2−(ISFS0+ITFS0)/2|=|0.03000 mm|. The difference (focus shift) between the average focus shift of the visible light in the three fields of view and the average focus shift of the infrared light in the three fields of view (RGB/IR) of the entire optical image capturing system is denoted by AFS (i.e. wavelength of 850 nm versus wavelength of 555 nm, unit of measurement: mm), for which the absolute value of |AIFS−AVFS|=|0.02800 mm| is satisfied.

In the optical image capturing system of the present embodiment, the modulation transfer rates (values of MTF) of the visible light at the quarter spatial frequency (110 cycles/mm) at the positions of the optical axis, 0.3 HOI and 0.7 HOT on the image plane are respectively denoted by MTFQ0, MTFQ3 and MTFQ7. The following conditions are satisfied: MTFQ0 is about 0.65, MTFQ3 is about 0.52 and MTFQ7 is about 0.42. The modulation transfer rates (values of MTF) at spatial frequency of 55 cycles/mm at the positions of the optical axis, 0.3 HOT and 0.7 HOT on the image plane are respectively denoted by MTFE0, MTFE3 and MTFE7. The following conditions are satisfied: MTFE0 is about 0.84, MTFE3 is about 0.76 and MTFE7 is about 0.69.

Please refer to FIG. 7. In the present embodiment, the optical image capturing system may include an image sensing device (not illustrated). The image sensor may include a substrate and an image sensor. The optical image capturing system may further include a first lens positioning element 710. The first lens positioning element may include a base and a lens base. The lens base may be disposed with an open accommodation space and may be disposed on the substrate, such that the image sensor may be accommodated in the accommodation space. The lens base, which may be integrally formed, may be hollow and opaque. The lens base may be disposed with a barrel portion 7141 and a base portion 7142 that are interconnected. The first hole 7143 and the second hole 7144 are respectively disposed at two opposite ends of the lens base. The first hole 7143 may be connected to the barrel portion 7141 and the second hole 7144 may be connected to the base portion 7142. The shortest side length of the base portion 7142, which is measured on a plane perpendicular to the optical axis, has a maximum value denoted by PhiD. The following condition is satisfied: PhiD=3.3 mm.

In the present embodiment, the optical image capturing system may further include a second lens positioning element 720. The second lens positioning element 720, which may include a positioning portion 722 and a connecting portion 724, may be accommodated in the lens base of the first lens positioning element 710. The positioning portion 722 may be hollow. A third hole 7241 and a fourth hole 7242 may be respectively disposed at two ends of the positioning portion 722 that are opposite to each other in the direction of the optical axis. The third hole 7241 may be connected to the positioning portion 722, and the fourth hole 7242 may be connected to the base portion 7142. The positioning portion 722 may come into direct contact with any lens element of the present embodiment. In addition, the positioning portion 722 is capable of accommodating the lens element and aligning the lens element on the optical axis. The connecting portion 724 may be disposed on the outer side of the positioning portion 722. The connecting portion 724 may directly couple with the barrel portion 7141 such that the second lens positioning element 720 can be accommodated in the lens base of the first lens positioning element, the optical image capturing system is capable of adjusting the focal length thereof along the optical axis, and the lens element can be positioned. The maximum outer diameter of the connecting portion 724 measured on a plane perpendicular to the optical axis is denoted by PhiC. The following condition is satisfied: PhiC=2.85 mm. The maximum inner diameter of the fourth hole 7242 is denoted by Phi4. The aforementioned connecting portion 724 may be disposed with screw threads, such that the second lens positioning element 720 and the lens base of the first lens positioning element 710 may be screwed together.

Any lens element in the present embodiment may be indirectly disposed in the first lens positioning element 710 through the second lens positioning element 720. Furthermore, the lens element may be nearer to the third hole 7241 than the image sensor, and the optical axis of the lens element may be perpendicular to the image sensor.

In the present embodiment, the fourth lens element 140 is closest to the image plane. The maximum effective diameter of the image-side surface thereof is denoted by PhiA4. The following condition is satisfied: PhiA=2 EHD42=1.767 mm. When the surface is aspheric, the terminal point of the curve defining the maximum effective diameter is the terminal point of the aspheric surface. The ineffective half diameter (IHD) of the image-side surface of the fourth lens element 140 is defined as the section of the image-side surface of the fourth lens element 140, in which the section extends, in a direction away from the optical axis, from the terminal point of the curve defining the maximum effective half diameter on the same surface. In the present embodiment, the fourth lens element 140 is closest to the image plane, and the maximum diameter of the image-side surface thereof is denoted by PhiB. The following condition is satisfied: PhiB=2 (EHD42+IHD)=PhiA4+2IHD=2.167 mm.

In the present embodiment, the maximum effective diameter of the image-side surface on the lens element that is closest to the image plane (i.e. image space) is the optical exit pupil of the optical image capturing system, which is denoted by PhiA4. The pupil magnification ratio is denoted by PMR, which may satisfy the following condition: PMR=PhiA4/HEP=1.84337. The exit pupil-image height ratio is denoted by PMMR, which may satisfy the following condition: PMMR=PhiA4/2HOI=0.58355. The miniaturization factor is denoted by PSMR, which may satisfy the following condition: PSMR=PhiA4/InTL=0.14269.

Table 1 and Table 2 below should be incorporated into the reference of the present embodiment.

TABLE 1 Lens Parameters for the First Embodiment f (focal length) = 2.6841 mm; f/HEP = 2.7959; HAF(half angle of view) = 70 deg; tan (HAF) = 2.7475 Surface Thickness Refractive Focal No. Curvature Radius (mm) Material Index Abbe No. Distance 0 Object Plane At infinity 1 Lens 1 31.98102785 0.918 Glass 1.688 50.26 −5.453 2 3.327880578 4.571 3 Lens 2 −15.2556818 2.500 Plastic 1.642 22.46 9.542 4 −4.681543531 2.528 5 Aperture Plane 0.225 Stop 6 Lens 3 −2.453543123 0.300 Plastic 1.642 22.46 −3.714 7 127.8664454 0.094 8 Lens 4 2.697747363 1.248 Plastic 1.544 56.09 2.759 9 −2.853715061 0.725 10 IR- Plane 2.000 BK7_SCHOTT 1.517 64.13 bandstop Filter 11 Plane 3.640 12 Image Plane Plane Reference Wavelength = 555 nm; Shield Position: The 3^(rd) surface with clear aperture of 3.0 mm

TABLE 2 Aspheric Coefficients of the First Embodiment Table 2: Aspheric Coefficients Surface No. 3 4 6 7 8 9 k = −2.918829E+01 −3.214789E+00 −1.504539E+01 −2.970417E+01 −1.613370E+01 −1.145951E+00 A₄ = −9.004096E−04 −9.725260E−06 8.890018E−05 3.634454E−02 9.587367E−03 −4.742020E−03 A₆ = 2.391364E−04 −8.096303E−05 −1.166688E−02 −3.060142E−02 −3.693991E−03 1.232422E−03 A₈ = −2.421089E−05 7.787465E−07 −5.720942E−04 8.833265E−03 8.653836E−04 3.333400E−04 A₁₀ = 1.716292E−06 3.517517E−07 8.305770E−04 −1.362695E−03 −7.093620E−05 −2.583094E−06 A₁₂ = 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

Table 1 is the detailed structural data for the first embodiment in FIG. 1A, wherein the unit for the curvature radius, the central thickness, the distance, and the focal length is millimeters (mm) Surfaces 0-11 illustrate the surfaces from the object side to the image plane in the optical image capturing system. Table 2 shows the aspheric coefficients of the first embodiment, wherein k is the conic coefficient in the aspheric surface equation, and A₁-A₂₀ are respectively the first to the twentieth order aspheric surface coefficients. Besides, the tables in the following embodiments correspond to their respective schematic views and the diagrams of aberration curves, and definitions of the parameters in these tables are similar to those in the Table 1 and the Table 2, so the repetitive details will not be given here.

Second Embodiment

Please refer to FIGS. 2A to 2E. FIG. 2A is a schematic view of the optical image capturing system according to the second embodiment of the present invention. FIG. 2B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system of the second embodiment, in the order from left to right. FIG. 2C is a characteristic diagram of the modulation transfer of visible light for the optical image capturing system of the second embodiment of the present invention. FIG. 2D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the second embodiment of the present invention. FIG. 2E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the second embodiment of the present disclosure. As shown in FIG. 2A, in the order from an object side to an image side, the optical image capturing system includes a first lens element 210, an aperture stop 200, a second lens element 220, a third lens element 230, a fourth lens element 240, an IR-bandstop filter 270, an image plane 280, and an image sensing device 290.

The first lens element 210 has negative refractive power and is made of plastic material. The first lens element 210 has a convex object-side surface 212 and a concave image-side surface 214. Both object-side surface 212 and image-side surface 214 are aspheric and have one inflection point.

The second lens element 220 has positive refractive power and is made of plastic material. The second lens element 220 has a convex object-side surface 222 and a convex image-side surface 224, and both object-side surface 222 and image-side surface 224 are aspheric. The object-side surface 222 thereof has one inflection point.

The third lens element 230 has positive refractive power and is made of plastic material. The third lens element 230 has a concave object-side surface 232 and a convex image-side surface 234, and both object-side surface 232 and image-side surface 234 are aspheric. Both object-side surface 232 and image-side surface 234 have one inflection point.

The fourth lens element 240 has negative refractive power and is made of plastic material. The fourth lens element 240 has a convex object-side surface 242 and a concave image-side surface 244, and both object-side surface 242 and image-side surface 244 are aspheric. The object-side surface 242 and image-side surface 244 thereof have one inflection point.

The IR-bandstop filter 270 is made of glass material and is disposed between the fourth lens element 240 and the image plane 280. The IR-bandstop filter 270 does not affect the focal length of the optical image capturing system.

In the optical image capturing system of the second embodiment, the second and third lens elements are positive lens, and their focal lengths are f2 and f3, respectively. The sum of the focal lengths for all lens elements having positive refractive power is ΣPP, which satisfies the following condition: ΣPP=f2+f3. Therefore, the positive refractive power of a single lens element may be distributed to other positive lens elements appropriately, so as to suppress noticeable aberrations generated when the incident light is propagating in the optical system.

In the optical image capturing system of the second embodiment, the sum of the focal lengths for all lens elements having negative refractive power is ΣNP, which satisfies the following condition: ΣNP=f1+f4.

Table 3 and Table 4 below should be incorporated into the reference of the present embodiment

TABLE 3 Lens Parameters for the Second Embodiment f(focal length) = 1.323 mm; f/HEP = 1.8; HAF(half angle of view) = 37.5 deg; tan(HAF) = 0.7673 Surface Thickness Refractive Abbe Focal No. Curvature Radius (mm) Material Index No. Length 0 Object Plane At infinity 1 Lens 1 2.815155869 0.175 Plastic 1.515 56.55 −4.014 2 1.16843349 0.051 3 Aperture Plane 0.066 Stop 4 Lens 2 0.599339272 0.450 Plastic 1.544 55.96 0.837 5 −1.411016917 0.133 6 Lens 3 −0.317760089 0.187 Plastic 1.642 22.46 5.004 7 −0.356324528 0.050 8 Lens 4 1.400960481 0.238 Plastic 1.642 22.46 −2.390 9 0.686143826 0.219 10 IR- Plane 0.210 BK7_SCHOTT 1.517 64.13 bandstop Filter 11 Plane 0.31 12 Image Plane Plane Reference Wavelength = 555 nm; Shield Position: The 1^(st) surface with clear aperture of 0.43 mm and the 5^(th) surface with clear aperture of 0.390 mm

TABLE 4 The Aspheric Coefficients of the Second Embodiment Table 4: Aspheric Coefficients Surface No. 1 2 4 5 6 7 k = −2.100896E+01 −3.117650E+01 −6.594072E−01 −5.749340E+00 −1.293538E+00 −1.778968E+00 A₄ = −1.034815E+00 −1.247743E+00 −2.144582E+00 −5.564182E−01 5.280891E+00 7.147752E+00 A₆= −1.467293E+01 −3.933644E+01 −2.397809E+01 −5.601046E+01 −4.929357E+01 −1.152802E+02 A₈ = 4.846220E+02 1.049222E+03 1.466540E+03 7.715029E+02 −5.524670E+02 1.188148E+03 A₁₀= −7.102825E+03 −1.234792E+04 −4.393327E+04 −8.580555E+03 2.181848E+04 −6.205622E+03 A₁₂ = 5.884002E+04 5.356074E+04 7.002153E+05 6.735915E+04 −2.298819E+05 2.212051E+04 A₁₄ = −2.820526E+05 1.558329E+05 −6.248007E+06 −2.902619E+05 1.176507E+06 −6.949962E+04 A₁₆ = 7.245452E+05 −2.134561E+06 2.912419E+07 5.267012E+05 −3.006163E+06 1.681686E+05 A₁₈ = −7.701193E+05 5.176547E+06 −5.535295E+07 −1.326747E+05 3.050941E+06 −1.906600E+05 A₂₀ = 1.874256E+01 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface No. 8 9 k = −9.958872E−02 −9.720777E+00 A₄ = 2.668792E+00 −6.993487E−01 A₆= −1.053723E+02 −9.822777E+00 A₈ = 1.164018E+03 9.374187E+01 A₁₀= −7.629138E+03 −4.377047E+02 A₁₂ = 3.098893E+04 1.160682E+03 A₁₄ = −7.777603E+04 −1.720966E+03 A₁₆ = 1.168351E+05 1.259258E+03 A₁₈ = −9.146103E+04 −3.228384E+02 A₂₀ = 0.000000E+00 0.000000E+00

In the second embodiment, the presentation of the aspheric surface equation is similar to that in the first embodiment. Besides, the definitions of parameters in following tables are similar to those in the first embodiment, so the repetitive details will not be given here.

The following values for the conditional expressions can be obtained from the data in Table 3 and Table 4.

Second Embodiment (Primary reference wavelength = 555 nm) ETP1 ETP2 ETP3 ETP4 ED12/ED23 SED 0.178  0.299  0.223  0.269  1.948  0.426  ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ED23/ED34 SETP 1.018  0.664  1.193  1.128  0.493  0.969  ETL EBL EIN EIR PIR STP 2.085  0.691  1.395  0.171  0.219  1.050  EIN/ETL SETP/EIN EIR/PIR EBL/BL BL SETP/STP 0.669  0.695  0.777  0.9344  0.7395  0.922  ED12 ED23 ED34 ED12/IN12 ED23/IN23 ED34/IN34 0.167  0.086  0.174  1.428  0.645  3.473  InRS41 InRS42 HVT41 HVT42 ODT % TDT % −0.02448   −0.00545   0.30907 0.42296 1.30002 0.70606 |f/f1| |f/f2| |f/f3| |f/f4| |f1/f2| |f2/f3| 0.32944 1.58025 0.26432 0.55346 4.79676 0.16726 ΣPPR ΣNPR ΣPPR/|ΣNPR| ΣPP ΣNP f1/ΣPP 1.84456 0.88290 2.08922 5.84043 −6.40396   −0.68735   f4/ΣNP IN12/f IN23/f IN34/f TP3/f TP4/f 0.37314 0.08827 0.10034 0.03781 0.14140 0.18018 InTL HOS HOS/HOI InS/HOS InTL/HOS ΣTP/InTL 1.34974 2.08923 2.03232 0.89196 0.64605 0.77815 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 0.64830 1.54164 0.38889 0.78476 0.17240 |InRS41|/TP4 |InRS42|/TP4 HVT42/HOI HVT42/HOS 0.1027  0.0229  0.4114  0.2024  MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.92   0.9   0.85   0.83   0.77   0.67   VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 0.00100 −0.00000   −0.00000   −0.00000   0.00250 0.00250 VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.63100 0.63600 0.59000 0.63100 0.60300 0.43700 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 0.01600 0.01250 0.00500 0.01500 0.01000 0.00250 ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.52100 0.44400 0.40200 0.52000 0.37400 0.19700 FS AIFS AVFS AFS PhiA4/InTL PhiA4/2HOI 0.01500 0.01000 0.00083 0.00917 1.0372  0.6809  PhiA4 PhiB PhiC PhiD PhiA4/HEP 1.4 mm 1.8 mm 2.2 mm 2.5 mm 1.9055 

The following values for the conditional expressions can be obtained from the data in Table 3 and Table 4.

Values Related to Inflection Point of Second Embodiment (Primary Reference Wavelength = 555 nm) HIF111 0.1522 HIF111/HOI 0.1481 SGI111 0.0034 |SGI111|/(|SGI111| + TP1) 0.0192 HIF121 0.1456 HIF121/HOI 0.1417 SGI121 0.0074 |SGI121|/(|SGI121| + TP1) 0.0408 HIF211 0.2328 HIF211/HOI 0.2264 SGI211 0.0389 |SGI211|/(|SGI211| + TP2) 0.0796 HIF311 0.2617 HIF311/HOI 0.2546 SGI311 −0.0900 |SGI311|/(|SGI311| + TP3) 0.3249 HIF321 0.2495 HIF321/HOI 0.2427 SGI321 −0.0673 |SGI321|/(|SGI321| + TP3) 0.2646 HIF411 0.1827 HIF411/HOI 0.1778 SGI411 0.0122 |SGI411|/(|SGI411| + TP4) 0.0486 HIF421 0.2076 HIF421/HOI 0.2020 SGI421 0.0250 |SGI421|/(|SGI421| + TP4) 0.0950

Third Embodiment

Please refer to FIGS. 3A to 3E. FIG. 3A is a schematic view of the optical image capturing system according to the third embodiment of the present invention. FIG. 3B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system, in the order from left to right, according to the third embodiment of the present invention. FIG. 3C is a characteristic diagram of modulation transfer of visible light spectrum for the optical image capturing system according to the third embodiment of the present invention. FIG. 3D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the third embodiment of the present invention. FIG. 3E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the third embodiment of the present disclosure. As shown in FIG. 3A, in the order from an object side to an image side, the optical image capturing system includes a first lens element 310, an aperture stop 300, a second lens element 320, a third lens element 330, a fourth lens element 340, an IR-bandstop filter 370, an image plane 380, and an image sensing device 390.

The first lens element 310 has positive refractive power and is made of plastic material. The first lens element 310 has a convex object-side surface 312 and a concave image-side surface 314, and both object-side surface 312 and image-side surface 314 are aspheric. Both of the object-side surface 312 and image-side surface 314 thereof have one inflection point.

The second lens element 320 has positive refractive power and is made of plastic material. The second lens element 320 has a convex object-side surface 322 and a convex image-side surface 324, and both object-side surface 322 and image-side surface 324 are aspheric. Both of the object-side surface 322 and image-side surface 324 thereof have one inflection point.

The third lens element 330 has positive refractive power and is made of plastic material. The third lens element 330 has a concave object-side surface 332 and a convex image-side surface 334, and both object-side surface 332 and image-side surface 334 are aspheric. Both of the object-side surface 332 and image-side surface 334 thereof have one inflection point.

The fourth lens element 340 has negative refractive power and is made of plastic material. The fourth lens element 340 has a convex object-side surface 342 and a concave image-side surface 344. Both object-side surface 342 and image-side surface 344 are aspheric and have one inflection point.

The IR-bandstop filter 370 is made of glass material and is disposed between the fourth lens element 340 and the image plane 380, without affecting the focal length of the optical image capturing system.

In the optical image capturing system of the third embodiment, the first, second and third lens elements are positive lens, and their focal lengths are f1, f2 and f3, respectively. The sum of the focal lengths for all lens elements having positive refractive power is ΣPP, which satisfies the following condition: ΣPP=f1+f2+f3. Therefore, the positive refractive power of a single lens element may be distributed to other positive lens elements appropriately, so as to suppress noticeable aberrations generated when the incident light is propagating in the optical system.

In the optical image capturing system of the third embodiment, the sum of the focal lengths for all lens elements having negative refractive power is ΣNP, which satisfies the following condition: ΣNP=f4.

Table 5 and Table 6 below should be incorporated into the reference of the present embodiment.

TABLE 5 Lens Parameters for the Third Embodiment f(focal length) = 1.3310 mm; f/HEP = 2.0; HAF(half angle of view) = 37.5170 deg; tan(HAF) = 0.7678 Surface Thickness Refractive Abbe Focal No. Curvature Radius (mm) Material Index No. Length 0 Object Plane At infinity 1 Lens 1 0.83935305 0.175 Plastic 1.584 29.88 238.535 2 0.779262354 0.085 3 Aperture Plane 0.050 Stop 4 Lens 2 0.623234619 0.285 Plastic 1.545 55.96 1.089 5 −11.00170615 0.123 6 Lens 3 −0.364938387 0.175 Plastic 1.642 22.46 10.040 7 −0.410676892 0.050 8 Lens 4 1.0692297 0.175 Plastic 1.642 22.46 −7.515 9 0.820249597 0.138 10 IR- Plane 0.210 BK7_SCHOTT 1.517 64.13 bandstop Filter 11 Plane 0.442 12 Image Plane Plane Reference Wavelength = 555 nm; Shield Position: The 1^(st) surface with clear aperture of 0.370 mm and the 5^(th) surface with clear aperture of 0.350 mm

TABLE 6 The Aspheric Coefficients of the Third Embodiment Table 6: Aspheric Coefficients Surface No. 1 2 4 5 6 7 k = −1.559670E+01 −3.285895E+01 −3.283737E−01 −2.715604E+01 −1.097425E+00 −1.384866E+00 A₄ = 2.960488E+00 5.065976E+00 −7.176660E−01 3.614461E−01 2.214305E+00 −4.780890E+00 A₆= −8.781953E+01 −1.155499E+02 −5.059534E+01 −7.045897E+01 −8.731178E+01 1.414294E+02 A₈ = 2.168917E+03 1.873961E+02 2.209574E+03 1.490315E+03 2.841182E+03 −1.711255E+03 A₁₀= −3.808808E+04 4.119672E+04 −6.239210E+04 −2.783463E+04 −5.162307E+04 9.272611E+03 A₁₂ = 4.172494E+05 −9.858251E+05 9.875788E+05 2.549608E+05 5.492447E+05 4.055356E+04 A₁₄ = −2.731712E+06 1.068435E+07 −9.081709E+06 −1.110874E+06 −3.054910E+06 −7.073760E+05 A₁₆ = 9.752197E+06 −5.730864E+07 4.401602E+07 2.625091E+06 7.919499E+06 2.992540E+06 A₁₈ = −1.459442E+07 1.229646E+08 −8.582584E+07 −4.104192E+06 −6.822180E+06 −4.349295E+06 A₂₀ = 1.874089E+01 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface No. 8 9 k = −9.000000E+01 −1.042971E+01 A₄ = −5.438650E+00 −5.344102E+00 A₆= 9.066051E+01 5.295146E+01 A₈ = −1.364068E+03 −4.481013E+02 A₁₀= 1.266697E+04 2.489477E+03 A₁₂ = −7.011162E+04 −8.594433E+03 A₁₄ = 2.041429E+05 1.680325E+04 A₁₆ = −2.001005E+05 −1.520673E+04 A₁₈ = −1.771508E+05 2.609779E+03 A₂₀ = 0.000000E+00 0.000000E+00

In the third embodiment, the presentation of the aspheric surface equation is similar to that in the first embodiment. Besides, the definitions of parameters in following tables are similar to those in the first embodiment, so the repetitive details will not be given here.

The following values for the conditional expressions can be obtained from the data in Table 5 and Table 6.

Third Embodiment (Primary Reference Wavelength = 555 nm) ETP1 ETP2 ETP3 ETP4 ED12/ED23 SED 0.162  0.193  0.186  0.197  3.763  0.351  ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ED23/ED34 SETP 0.926  0.679  1.062  1.126  0.272  0.738  ETL EBL EIN EIR PIR STP 2.085  0.691  1.395  0.171  0.219  0.810  EIN/ETL SETP/EIN EIR/PIR EBL/BL BL SETP/STP 0.669  0.695  0.777  0.8747  0.79   0.912  ED12 ED23 ED34 ED12/IN12 ED23/IN23 ED34/IN34 0.157  0.042  0.153  1.164  0.339  3.061  InRS41 InRS42 HVT41 HVT42 ODT % TDT % −0.06700   −0.09200   0.20300 0.29700 1.30000 0.60800 |f/f1| |f/f2| |f/f3| |f/f4| |f1/f2| |f2/f3| 0.00558 1.22222 0.13257 0.17711 219.04040  0.10847 ΣPPR ΣNPR ΣPPR/|ΣNPR| ΣPP ΣNP f1/ΣPP 1.36037 0.17711 7.68084 249.66400  −7.51500   0.95542 f4/ΣNP IN12/f IN23/f IN34/f TP3/f TP4/f −0.14491   0.10143 0.09241 0.03757 0.13148 0.13148 InTL HOS HOS/HOI InS/HOS InTL/HOS ΣTP/InTL 1.11700 1.90700 1.85506 0.86418 0.58574 0.72516 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 1.08772 1.28571 0.61404 1.00000 0.21098 |InRS41|/TP4 |InRS42|/TP4 HVT42/HOI HVT42/HOS 0.3829  0.5257  0.2889  0.1557  MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.9   0.86   0.8   0.76   0.65   0.54   VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 0.00250 −0.00000   −0.00750   0.00250 0.00750 0.01000 VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.53300 0.52000 0.51900 0.53300 0.48200 0.40700 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 0.02250 0.01750 0.00500 0.02250 0.02250 0.00750 ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.52000 0.43000 0.39200 0.52000 0.34700 0.20200 FS AIFS AVFS AFS PhiA4/InTL PhiA4/2HOI 0.02000 0.01625 0.00250 0.01375 1.0743  0.5837  PhiA4 PhiB PhiC PhiD PhiA4/HEP 1.2 mm 1.6 mm 2.0 mm 2.3 mm 1.8032 

The following values for the conditional expressions can be obtained from the data in Table 5 and Table 6.

Values Related to Inflection Point of Third Embodiment (Primary Reference Wavelength = 555 nm) HIF111 0.2660 HIFI11/HOI 0.2588 SGI111 0.0370 |SGI111|/(|SGI111| + TP1) 0.1745 HIF121 0.1940 HIF121/HOI 0.1887 SGI121 0.0200 |SGI121|/(|SGI121| + TP1) 0.1026 HIF211 0.2270 HIF211/HOI 0.2208 SGI211 0.0380 |SGI211|/(|SGI211| + TP2) 0.1176 HIF221 0.3430 HIF221/HOI 0.3337 SGI221 −0.0490 |SGI221|/(|SGI221| + TP2) 0.1467 HIF311 0.2590 HIF311/HOI 0.2519 SGI311 −0.0860 |SGI311|/(|SGI311| + TP3) 0.3295 HIF321 0.2470 HIF321/HOI 0.2403 SGI321 −0.0730 |SGI321|/(|SGI321| + TP3) 0.2944 HIF411 0.0950 HIF411/HOI 0.0924 SGI411 0.0030 |SGI411|/(|SGI411| + TP4) 0.0169 HIF421 0.1440 HIF421/HOI 0.1401 SGI421 0.0100 |SGI421|/(|SGI421| + TP4) 0.0541

Fourth Embodiment

Please refer to FIGS. 4A to 4E. FIG. 4A is a schematic view of the optical image capturing system according to the fourth embodiment of the present invention. FIG. 4B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system, in the order from left to right, according to the fourth embodiment of the present invention. FIG. 4C is a characteristic diagram of modulation transfer of visible light spectrum for the optical image capturing system according to the fourth embodiment of the present invention. FIG. 4D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fourth embodiment of the present invention. FIG. 4E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fourth embodiment of the present disclosure. As shown in FIG. 4A, in the order from an object side to an image side, the optical image capturing system includes a first lens element 410, an aperture stop 400, a second lens element 420, a third lens element 430, a fourth lens element 440, an IR-bandstop filter 470, an image plane 480, and an image sensing device 490.

The first lens element 410 has positive refractive power and is made of plastic material. The first lens element 410 has a convex object-side surface 412 and a concave image-side surface 414, and both object-side surface 412 and image-side surface 414 are aspheric. Both of the object-side surface 412 and image-side surface 414 thereof have an inflection point.

The second lens element 420 has positive refractive power and is made of plastic material. The second lens element 420 has a convex object-side surface 422 and a convex image-side surface 424, and both object-side surface 422 and image-side surface 424 are aspheric. The object-side surface 422 thereof has an inflection point.

The third lens element 430 has negative refractive power and is made of plastic material. The third lens element 430 has a concave object-side surface 432 and a convex image-side surface 434, and both object-side surface 432 and image-side surface 434 are aspheric. The object-side surface 432 and image-side surface 434 thereof both have an inflection point.

The fourth lens element 440 has positive refractive power and is made of plastic material. The fourth lens element 440 has a convex object-side surface 442 and a concave image-side surface 444. Both object-side surface 442 and image-side surface 444 are aspheric and have an inflection point.

The IR-bandstop filter 470 is made of glass material and is disposed between the fourth lens element 440 and the image plane 480, without affecting the focal length of the optical image capturing system.

In the optical image capturing system of the fourth embodiment, the first, second and fourth lens elements are positive lens, and their focal lengths are f1, f2 and f4, respectively. The sum of the focal lengths for all lens elements having positive refractive power is ΣPP, which satisfies the following condition: ΣPP=f1+f2+f4. Therefore, the positive refractive power of a single lens element may be distributed to other positive lens elements appropriately, so as to suppress noticeable aberrations generated when the incident light is propagating in the optical system.

In the optical image capturing system of the fourth embodiment, the focal length of the third lens element is f3, and the sum of the focal lengths for all lens elements having negative refractive power is ΣNP, which satisfies the following condition: ΣNP=f3.

Table 7 and Table 8 below should be incorporated into the reference of the present embodiment.

TABLE 7 Lens Parameters for the Fourth Embodiment f(focal length) = 1.3290 mm; f/HEP = 2.0; HAF(half angle of view) = 37.5150 deg; tan(HAF) = 0.7677 Surface Thickness Refractive Abbe Focal No. Curvature Radius (mm) Material Index No. Length 0 Object Plane At infinity 1 Lens 1 0.796358327 0.175 Plastic 1.584 29.88 47.93 2 0.752894203 0.095 3 Aperture Plane 0.050 Stop 4 Lens 2 0.69002414 0.289 Plastic 1.545 55.96 1.14 5 −5.470145447 0.127 6 Lens 3 −0.375226684 0.175 Plastic 1.642 22.46 −7.54 7 −0.480949837 0.050 8 Lens 4 0.634776701 0.175 Plastic 1.642 22.46 9.92 9 0.628050498 0.130 10 IR- Plane 0.210 BK7_SCHOTT 1.517 64.13 bandstop Filter 11 Plane 0.446 12 Image Plane Plane Reference Wavelength = 555 nm; Shield Position: The 1^(st) surface with clear aperture of 0.390 mm and the 5^(th) surface with clear aperture of 0.350 mm

TABLE 8 The Aspheric Coefficients of the Fourth Embodiment Table 8: Aspheric Coefficients Surface No. 1 2 4 5 6 7 k = −1.559070E+01 −3.277696E+01 −1.338964E−01 −2.644155E+01 −9.444825E−01 −8.569895E−01 A₄ = 3.931058E+00 6.407587E+00 −7.455663E−01 −3.112638E−01 1.474769E+00 −7.584700E+00 A₆= −1.040453E+02 −1.208225E+02 −4.905075E+01 −7.316173E+01 −2.913984E+01 2.026719E+02 A₈ = 2.548788E+03 −4.252993E+01 2.152711E+03 1.536768E+03 1.861605E+02 −2.697091E+03 A₁₀= −4.367449E+04 4.938506E+04 −6.180943E+04 −3.005936E+04 −1.107176E+03 1.921504E+04 A₁₂ = 4.647813E+05 −1.098966E+06 9.823348E+05 3.189116E+05 8.405416E+04 −1.663989E+04 A₁₄ = −2.944070E+06 1.140707E+07 −9.044375E+06 −1.714189E+06 −9.804138E+05 −5.393357E+05 A₁₆ = 1.013712E+07 −5.908647E+07 4.382259E+07 4.420446E+06 4.316120E+06 2.803448E+06 A₁₈ = −1.459442E+07 1.229646E+08 −8.582584E+07 −4.104192E+06 −6.822180E+06 −4.349295E+06 A₂₀ = 1.874407E+01 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface No. 8 9 k = −2.727253E+01 −1.028315E+01 A₄ = −4.999799E+00 −3.743632E+00 A₆= 6.751631E+01 2.859772E+01 A₈ = −9.280684E+02 −2.281186E+02 A₁₀= 7.954824E+03 1.278101E+03 A₁₂ = −3.875688E+04 −4.522034E+03 A₁₄ = 8.940373E+04 9.165264E+03 A₁₆ = −2.453740E+04 −9.062636E+03 A₁₈ = −1.771508E+05 2.609779E+03 A₂₀ = 0.000000E+00 0.000000E+00

In the fourth embodiment, the form of the aspheric surface equation is similar to that in the first embodiment. Besides, the definitions of parameters in following tables are similar to those in the first embodiment, so the repetitive details will not be given here.

The following values for the conditional expressions can be obtained from the data in Table 7 and Table 8.

Fourth Embodiment (Primary Reference Wavelength = 555 nm) ETP1 ETP2 ETP3 ETP4 ED12/ED23 SED 0.165 0.200 0.190 0.192 2.891 0.369 ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ED23/ED34 SETP 0.941 0.692 1.088 1.096 0.308 0.747 ETL EBL EIN EIR PIR STP 1.869 0.753 1.116 0.096 0.130 0.814 EIN/ETL SETP/EIN EIR/PIR EBL/BL BL SETP/STP 0.597 0.670 0.742  0.9568 0.787 0.918 ED12 ED23 ED34 ED12/IN12 ED23/IN23 ED34/IN34 0.149 0.052 0.168 1.028 0.408 3.356 InRS41 InRS42 HVT41 HVT42 ODT % TDT %  −0.04300  −0.06200  0.26100  0.34000  1.30500  0.49200 |f/f1| |f/f2| |f/f3| |f/f4| |f1/f2| |f2/f3|  0.02773  1.16477  0.17617  0.13399  42.00876  0.15125 ΣPPR ΣNPR ΣPPR/|ΣNPR| ΣPP ΣNP f1/ΣPP  1.32648  0.17617  7.52969  58.99200  −7.54400  0.81252 f4/ΣNP IN12/f IN23/f IN34/f TP3/f TP4/f  −0.15125  0.10910  0.09556  0.03762  0.13168  0.13168 InTL HOS HOS/HOI InS/HOS InTL/HOS ΣTP/InTL  1.13600  1.92300  1.87062  0.85959  0.59074  0.71655 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3)  1.10727  1.28571  0.60554  1.00000 0.21489 |InRS41|/TP4 |InRS42|/TP4 HVT42/HOI HVT42/HOS  0.2457  0.3543  0.3307  0.1768 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.9  0.87  0.84  0.75  0.68  0.58  VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 0.003 −0.000   −0.008   0.003 0.008 0.008 VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.525 0.532 0.540 0.525 0.514 0.418 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 0.025 0.020 0.005 0.025 0.020 0.008 ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.519 0.440 0.400 0.519 0.368 0.214 FS AIFS AVFS AFS PhiA4/InTL PhiA4/2HOI 0.023 0.017 0.002 0.015  1.1004  0.6080 PhiA4 PhiB PhiC PhiD PhiA4/HEP 1.25 mm 1.65 mm 2.05 mm 2.35 mm  1.8811

The following values for the conditional expressions can be obtained from the data in Table 7 and Table 8.

Values Related to Inflection Point of Fourth Embodiment (Primary Reference Wavelength = 555 nm) HIF111 0.3010 HIF111/HOI 0.2928 SGI111 0.0510 |SGI111|/(|SGI111| + TP1) 0.2257 HIF121 0.2200 HIF121/HOI 0.2140 SGI121 0.0280 |SGI121|/(|SGI121| + TP1) 0.1379 HIF211 0.2190 HIF211/HOI 0.2130 SGI211 0.0320 |SGI211|/(|SGI211| + TP2) 0.0997 HIF311 0.2600 HIF311/HOI 0.2529 SGI311 −0.0870 |SGI311|/(|SGI311| + TP3) 0.3321 HIF321 0.2570 HIF321/HOI 0.2500 SGI321 −0.0750 |SGI321|/(|SGI321| + TP3) 0.3000 HIF411 0.1210 HIF411/HOI 0.1177 SGI411 0.0090 |SGI411|/(|SGI411| + TP4) 0.0489 HIF421 0.1620 HIF421/HOI 0.1576 SGI421 0.0160 |SGI421|/(|SGI421| + TP4) 0.0838

Fifth Embodiment

Please refer to FIGS. 5A to 5E. FIG. 5A is a schematic view of the optical image capturing system according to the fifth embodiment of the present invention. FIG. 5B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system, in the order from left to right, according to the fifth embodiment of the present invention. FIG. 5C is a characteristic diagram of modulation transfer of visible light spectrum for the optical image capturing system according to the fifth embodiment of the present invention. FIG. 5D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fifth embodiment of the present invention. FIG. 5E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fifth embodiment of the present disclosure. As shown in FIG. 5A, in the order from an object side to an image side, the optical image capturing system includes a first lens element 510, an aperture stop 500, a second lens element 520, a third lens element 530, a fourth lens element 540, an IR-bandstop filter 570, an image plane 580, and an image sensing device 590.

The first lens element 510 has positive refractive power and is made of plastic material. The first lens element 510 has a convex object-side surface 512 and a concave image-side surface 514, and both object-side surface 512 and image-side surface 514 are aspheric. The object-side surface 512 and image-side surface 514 thereof both have one inflection point.

The second lens element 520 has positive refractive power and is made of plastic material. The second lens element 520 has a convex object-side surface 522 and a convex image-side surface 524, and both object-side surface 522 and image-side surface 524 are aspheric. The object-side surface 522 thereof has one inflection point.

The third lens element 530 has positive refractive power and is made of plastic material. The third lens element 530 has a concave object-side surface 532 and a convex image-side surface 534, and both object-side surface 532 and image-side surface 534 are aspheric. The object-side surface 532 and image-side surface 534 thereof both have one inflection point.

The fourth lens element 540 has negative refractive power and is made of plastic material. The fourth lens element 540 has a convex object-side surface 542 and a concave image-side surface 544. Both object-side surface 542 and image-side surface 544 are aspheric. The object-side surface 542 and image-side surface 544 thereof both have one inflection point.

The IR-bandstop filter 570 is made of glass material and is disposed between the fourth lens element 540 and the image plane 580, without affecting the focal length of the optical image capturing system.

In the optical image capturing system of the fifth embodiment, the first, second and third lens elements are positive lens, and their focal lengths are f1, f2 and f3, respectively. The sum of the focal lengths for all lens elements having positive refractive power is ΣPP, which satisfies the following condition: ΣPP=f1+f2+f3. Therefore, the positive refractive power of a single lens element may be distributed to other positive lens elements appropriately, so as to suppress noticeable aberrations generated when the incident light is propagating in the optical system.

In the optical image capturing system of the fifth embodiment, the sum of the focal lengths for all lens elements having negative refractive power is ΣNP, which satisfies the following condition: ΣNP=f4.

Table 9 and Table 10 below should be incorporated into the reference of the present embodiment.

TABLE 9 Lens Parameters for the Fifth Embodiment f(focal length) = 1.3290 mm; f/HEP = 2.0; HAF(half angle of view) = 37.5120 deg; tan(HAF) = 0.7677 Surface Thickness Refractive Abbe Focal No. Curvature Radius (mm) Material Index No. Length 0 Object Plane At Infinity 1 Lens 1 0.764838324 0.175 Plastic 1.584 29.88 32.549 2 0.729251375 0.105 3 Aperture Plane 0.050 Stop 4 Lens 2 0.770395463 0.297 Plastic 1.545 55.96 1.164 5 −3.142770862 0.142 6 Lens 3 −0.364018853 0.175 Plastic 1.642 22.46 10.785 7 −0.411367225 0.050 8 Lens 4 0.704534047 0.175 Plastic 1.642 22.46 −8.882 9 0.566378176 0.133 10 IR- Plane 0.210 BK_7 1.517 64.13 bandstop Filter 11 Plane 0.426 12 Image Plane 0.000 Plane Reference Wavelength = 555 nm; Shield Position: The 1^(st) surface with clear aperture of 0.400 mm and the 5^(th) surface with clear aperture of 0.350 mm

TABLE 10 The Aspheric Coefficients of the Fifth Embodiment Table 10: Aspheric Coefficients Surface No. 1 2 4 5 6 7 k = −1.556135E+01 −3.280664E+01 −3.827055E−01 −2.644155E+01 −9.330802E−01 −1.025218E+00 A₄ = 4.702703E+00 7.815202E+00 −7.484692E−01 −1.194821E+00 2.840791E−01 −4.611834E+00 A₆= −1.160799E+02 −1.393947E+02 −3.722463E+01 −5.746811E+01 2.103726E+01 1.376837E+02 A₈ = 2.832783E+03 2.293905E+02 1.632621E+03 1.097333E+03 −1.663331E+03 −1.900876E+03 A₁₀= −4.795248E+04 4.713187E+04 −5.067966E+04 −2.273134E+04 3.161881E+04 1.231873E+04 A₁₂ = 5.017520E+05 −1.090364E+06 8.450075E+05 2.609284E+05 −2.054994E+05 2.342849E+04 A₁₄ = −3.109684E+06 1.139193E+07 −8.139072E+06 −1.526369E+06 2.733846E+05 −6.727018E+05 A₁₆ = 1.043435E+07 −5.906522E+07 4.116555E+07 4.236962E+06 2.190178E+06 2.990921E+06 A₁₈ = −1.459442E+07 1.229646E+08 −8.582584E+07 −4.104192E+06 −6.822180E+06 −4.349295E+06 A₂₀ = 1.874596E+01 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface No. 8 9 k = −3.602467E+01 −1.030472E+01 A₄ = −2.350703E+00 −2.912683E+00 A₆= 1.381331E+01 1.830157E+01 A₈ = −2.230149E+02 −1.401876E+02 A₁₀= 1.983758E+03 7.950709E+02 A₁₂ = −7.402581E+03 −2.878355E+03 A₁₄ = −2.462934E+03 6.062118E+03 A₁₆ = 9.002743E+04 −6.575243E+03 A₁₈ = −1.771508E+05 2.609779E+03 A₂₀ = 0.000000E+00 0.000000E+00

In the fifth embodiment, the form of the aspheric surface equation is similar to that in the first embodiment. Besides, the definitions of parameters in following tables are similar to those in the first embodiment, so the repetitive details will not be given here.

The following values for the conditional expressions can be obtained from the data in Table 9 and Table 10:

Fifth Embodiment (Primary Reference Wavelength = 555 nm) ETP1 ETP2 ETP3 ETP4 ED12/ED23 SED 0.167 0.210 0.188 0.196 2.088 0.389 ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ED23/ED34 SETP 0.957 0.707 1.075 1.120 0.380 0.761 ETL EBL EIN EIR PIR STP 1.879 0.729 1.150 0.093 0.133 0.822 EIN/ETL SETP/EIN EIR/PIR EBL/BL BL SETP/STP 0.612 0.662 0.703  0.9480 0.769 0.927 ED12 ED23 ED34 ED12/IN12 ED23/IN23 ED34/IN34 0.142 0.068 0.179 0.916 0.479 3.577 InRS41 InRS42 HVT41 HVT42 ODT % TDT %  −0.04100  −0.04600  0.27400  0.36500  1.30000  0.44600 |f/f1| |f/f2| |f/f3| |f/f4| |f1/f2| |f2/f3|  0.04083  1.14175  0.12323  0.14963  27.96306  0.10793 ΣPPR ΣNPR ΣPPR/|ΣNPR| ΣPP ΣNP f1/ΣPP  1.30581  0.14963  8.72702  44.49800  −8.88200  0.73147 f4/ΣNP IN12/f IN23/f IN34/f TP3/f TP4/f  1.00000  0.11663  0.10685  0.03762  0.13168  0.13168 InTL HOS HOS/HOI InS/HOS InTL/HOS ΣTP/InTL  1.16800  1.93700  1.88424  0.85545  0.60299  0.70377 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3)  1.11111  1.28571  0.58923  1.00000 0.23127 |InRS41|/TP4 |InRS42|/TP4 HVT42/HOI HVT42/HOS  0.2343  0.2629  0.3551  0.1884 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.9  0.89  0.85  0.75  0.73  0.64  VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 0.003 −0.000   −0.005   0.003 0.005 0.005 VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.506 0.529 0.555 0.506 0.535 0.434 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 0.025 0.020 0.008 0.025 0.020 0.008 ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.527 0.458 0.408 0.527 0.392 0.222 FS AIFS AVFS AFS PhiA4/InTL PhiA4/2HOI 0.023 0.018 0.002 0.016  1.1130  0.6323 PhiA4 PhiB PhiC PhiD PhiA4/HEP 1.3 mm 1.7 mm 2.1 mm 2.4 mm  1.9564

The following values for the conditional expressions can be obtained from the data in Table 9 and Table 10.

Values Related to Inflection Point of Fifth Embodiment (Primary Reference Wayelength = 555 nm) HIF111 0.3250 HIF111/HOI 0.3161 SGI111 0.0640 |SGI111|/(|SGI111| + TP1) 0.2678 HIF121 0.2410 HIF121/HOI 0.2344 SGI121 0.0350 |SGI121|/(|SGI121| + TP1) 0.1667 HIF211 0.2080 HIF211/HOI 0.2023 SGI211 0.0260 |SGI211|/(|SGI211| + TP2) 0.0805 HIF311 0.2620 HIF311/HOI 0.2549 SGI311 −0.0950 |SGI311|/(|SGI311| + TP3) 0.3519 HIF321 0.2640 HIF321/HOI 0.2568 SGI321 −0.0860 |SGI321|/(|SGI321| + TP3) 0.3295 HIF411 0.1330 HIF411/HOI 0.1294 SGI411 0.0090 |SGI411|/(|SGI411| + TP4) 0.0489 HIF421 0.1710 HIF421/HOI 0.1663 SGI421 0.0200 |SGI421|/(|SGI421| + TP4) 0.1026

Sixth Embodiment

Please refer to FIGS. 6A to 6E. FIG. 6A is a schematic view of the optical image capturing system according to the sixth embodiment of the present invention. FIG. 6B shows the longitudinal spherical aberration curves, astigmatic field curves, and optical distortion curve of the optical image capturing system, in the order from left to right, according to the sixth embodiment of the present invention. FIG. 6C is a characteristic diagram of modulation transfer of visible light spectrum for the optical image capturing system according to the sixth embodiment of the present invention. FIG. 6D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the sixth embodiment of the present invention. FIG. 6E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the sixth embodiment of the present disclosure. As shown in FIG. 6A, in the order from an object side to an image side, the optical image capturing system includes a first lens element 610, an aperture stop 600, a second lens element 620, a third lens element 630, a fourth lens element 640, an IR-bandstop filter 670, an image plane 680, and an image sensing device 690.

The first lens element 610 has positive refractive power and is made of plastic material. The first lens element 610 has a convex object-side surface 612 and a concave image-side surface 614, and both object-side surface 612 and image-side surface 614 are aspheric. The object-side surface 612 thereof has an inflection point.

The second lens element 620 has positive refractive power and is made of plastic material. The second lens element 620 has a convex object-side surface 622 and a convex image-side surface 624, and both object-side surface 622 and image-side surface 624 are aspheric. The object-side surface 622 thereof has one inflection points.

The third lens element 630 has positive refractive power and is made of plastic material. The third lens element 630 has a concave object-side surface 632 and a convex image-side surface 634, and both object-side surface 632 and image-side surface 634 are aspheric. The object-side surface 632 thereof has one inflection points.

The fourth lens element 640 has negative refractive power and is made of plastic material. The fourth lens element 640 has a convex object-side surface 642 and a concave image-side surface 644. Both object-side surface 642 and image-side surface 644 are aspheric and have one inflection point.

The IR-bandstop filter 670 is made of glass material and is disposed between the fourth lens element 640 and the image plane 680, without affecting the focal length of the optical image capturing system.

In the optical image capturing system of the sixth embodiment, the first, second and third lens elements are positive lens, and their focal lengths are f1, f2 and f3, respectively. The sum of the focal lengths for all lens elements having positive refractive power is ΣPP, which satisfies the following condition: ΣPP=f1+f2+f3. Therefore, the positive refractive power of a single lens element may be distributed to other positive lens elements appropriately, so as to suppress noticeable aberrations generated when the incident light is propagating in the optical system.

In the optical image capturing system of the sixth embodiment, the sum of the focal lengths for all lens elements having negative refractive power is ΣNP, which satisfies the following condition: ΣNP=f4.

Table 11 and Table 12 below should be incorporated into the reference of the present embodiment.

TABLE 11 Lens Parameters for the Sixth Embodiment f(focal length) = 1.3290 mm; f/HEP = 2.0; HAF(half angle of view) = 37.5120 deg; tan(HAF) = 0.7677 Surface Thickness Refractive Abbe Focal No. Curvature Radius (mm) Material Index No. Length 0 Object Plane At infinity 1 Lens 1 0.852727177 0.175 Plastic 1.584 29.88 27.43 2 0.831996164 0.091 3 Aperture Plane 0.054 Stop 4 Lens 2 0.761891411 0.289 Plastic 1.545 55.96 1.19 5 −3.904738276 0.165 6 Lens 3 −0.361643479 0.175 Plastic 1.642 22.46 3.29 7 −0.367957202 0.050 8 Lens 4 0.829526508 0.175 Plastic 1.642 22.46 −3.09 9 0.537691373 0.133 10 IR- Plane 0.210 BK_7 1.517 64.13 bandsop Filter 11 Plane 0.403 12 Image Plane Plane Reference Wavelength = 555 nm; Shield Position: The 1^(st) surface with clear aperture of 0.410 mm and the 5^(th) surface with clear aperture of 0.390 mm

TABLE 12 The Aspheric Coefficients of the Sixth Embodiment Table 12: Aspheric Coefficients Surface No. 1 2 4 5 6 7 k = −1.557647E+01 −3.277776E+01 −2.789439E−01 −2.836680E+01 −8.227774E−01 −1.160439E+00 A₄ = 3.496099E+00 4.070620E+00 −1.045470E+00 −1.071473E+00 −7.042761E−02 −1.595838E+00 A₆= −1.127991E+02 −3.227539E+01 −2.564283E+01 −5.128397E+01 4.173408E+01 5.861257E+01 A₈ = 3.028273E+03 −2.350251E+03 1.176839E+03 1.010546E+03 −2.176985E+03 −6.395381E+02 A₁₀= −5.234801E+04 8.785110E+04 −3.996886E+04 −2.036338E+04 3.762443E+04 −1.481922E+03 A₁₂ = 5.430169E+05 −1.475501E+06 7.157242E+05 2.273671E+05 −2.413331E+05 1.134396E+05 A₁₄ = −3.294190E+06 1.338238E+07 −7.321641E+06 −1.326611E+06 3.738232E+05 −9.795245E+05 A₁₆ = 1.075724E+07 −6.336433E+07 3.923895E+07 3.816418E+06 2.097561E+06 3.407940E+06 A₁₈ = −1.459442E+07 1.229646E+08 −8.582584E+07 −4.104192E+06 −6.822180E+06 −4.349295E+06 A₂₀ = 1.874288E+01 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface No. 8 9 k = −5.134444E+01 −1.033455E+01 A₄ = −4.577708E−01 −2.412686E+00 A₆= −1.934862E+01 1.478557E+01 A₈ = 1.955137E+02 −1.211551E+02 A₁₀= −1.529580E+03 7.099192E+02 A₁₂ = 1.081871E+04 −2.582762E+03 A₁₄ = −5.450324E+04 5.449786E+03 A₁₆ = 1.527241E+05 −6.031428E+03 A₁₈ = −1.771508E+05 2.609779E+03 A₂₀ = 0.000000E+00 0.000000E+00

In the sixth embodiment, the form of the aspheric surface equation is similar to that in the first embodiment. Besides, the definitions of parameters in following tables are similar to those in the first embodiment, so the repetitive details will not be given here.

The following values for the conditional expressions can be obtained from the data in Table 11 and Table 12:

Sixth Embodiment (Primary Reference Wavelength = 555 nm) ETP1 ETP2 ETP3 ETP4 ED12/ED23 SED 0.164 0.203 0.185 0.201 1.841 0.415 ETP1/TP1 ETP2/TP2 ETP3/TP3 ETP4/TP4 ED23/ED34 SETP 0.939 0.702 1.059 1.147 0.419 0.753 ETL EBL EIN EIR PIR STP 1.870 0.702 1.168 0.089 0.133 0.814 EIN/ETL SETP/EIN EIR/PIR EBL/BL BL SETP/STP 0.624 0.645 0.668  0.9398 0.747 0.925 ED12 ED23 ED34 ED12/IN12 ED23/IN23 ED34/IN34 0.146 0.079 0.189 1.006 0.481 3.786 InRS41 InRS42 HVT41 HVT42 ODT % TDT %  −0.04000  −0.03700  0.28600  0.38800  1.30600  0.56600 |f/f1| |f/f2| |f/f3| |f/f4| |f1/f2| |f2/f3|  0.04845  1.11400  0.40407  0.43038  22.99413  0.36272 ΣPPR ΣNPR ΣPPR/|ΣNPR| ΣPP ΣNP f1/ΣPP  1.56652  0.43038  3.63989  31.91400  −3.08800  0.85956 f4/ΣNP IN12/f IN23/f IN34/f TP3/f TP4/f  1.00000  0.10910  0.12415  0.03762  0.13168  0.13168 InTL HOS HOS/HOI InS/HOS InTL/HOS ΣTP/InTL  1.17400  1.92100  1.86868  0.86101  0.61114  0.69336 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3)  1.10727  1.28571  0.60554  1.00000 0.26232 |InRS41|/TP4 |InRS42|/TP4 HVT42/HOI HVT42/HOS  0.2286  0.2114  0.3774  0.2020 MTFE0 MTFE3 MTFE7 MTFQ0 MTFQ3 MTFQ7 0.9  0.88  0.85  0.73  0.74  0.65  VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 0.003 −0.000   −0.005   0.003 0.005 0.005 VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.506 0.529 0.555 0.506 0.535 0.434 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 0.025 0.020 0.008 0.025 0.020 0.008 ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.527 0.458 0.408 0.527 0.392 0.222 FS AIFS AVFS AFS PhiA4/InTL PhiA4/2HOI 0.023 0.018 0.002 0.016  1.1499  0.6566 PhiA4 PhiB PhiC PhiD PhiA4/HEP 1.35 mm 1.75 mm 2.15 mm 2.45 mm  2.0316

The following values for the conditional expressions can be obtained from the data in Table 11 and Table 12:

Values Related to Inflection Point of Sixth Embodiment (Primary Reference Wavelength = 555 nm) HIF111 0.3020 HIF111/HOI 0.2938 SGI111 0.0470 |SGI111|/(|SGI111| + TP1) 0.2117 HIF121 0.2210 HIF121/HOI 0.2150 SGI121 0.0250 |SGI121|/(|SGI121| + TP1) 0.1250 HIF211 0.2120 HIF211/HOI 0.2062 SGI211 0.0270 |SGI211|/(|SGI211| + TP2) 0.0854 HIF311 0.2670 HIF311/HOI 0.2597 SGI311 −0.1010 |SGI311|/(|SGI311| + TP3) 0.3659 HIF321 0.2720 HIF321/HOI 0.2646 SGI321 −0.0960 |SGI321|/(|SGI321| + TP3) 0.3542 HIF411 0.1460 HIF411/HOI 0.1420 SGI411 0.0090 |SGI411|/(|SGI411| + TP4) 0.0489 HIF421 0.1790 HIF421/HOI 0.1741 SGI421 0.0230 |SGI421|/(|SGI421| + TP4) 0.1162

Although the present invention is disclosed by the aforementioned embodiments, those embodiments do not serve to limit the scope of the present invention. A person skilled in the art could perform various alterations and modifications to the present invention, without departing from the spirit and the scope of the present invention. Hence, the scope of the present invention should be defined by the following appended claims.

Despite the fact that the present invention is specifically presented and illustrated with reference to the exemplary embodiments thereof, it should be apparent to a person skilled in the art that, various modifications could be performed to the forms and details of the present invention, without departing from the scope and spirit of the present invention defined in the claims and their equivalence. 

What is claimed is:
 1. An optical image capturing system, from an object side to an image side, comprising: a first lens element with refractive power; a second lens element with refractive power; a third lens element with refractive power; a fourth lens element with refractive power; a first image plane, which is an image plane specifically for visible light and perpendicular to an optical axis; a through-focus modulation transfer rate (value of MTF) at a first spatial frequency having a maximum value at central field of view of the first image plane; and a second image plane, which is an image plane specifically for infrared light and perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency having a maximum value at central of field of view of the second image plane, wherein the optical image capturing system comprises four lens elements with refractive powers, at least one of the four lens elements has positive refractive power; focal lengths of the four lens elements are respectively f1, f2, f3 and f4; a focal length of the optical image capturing system is f, and an entrance pupil diameter of the optical image capturing system is HEP; a distance on the optical axis from an object-side surface of the first lens element to the first image plane is HOS, a distance on the optical axis from the object-side surface of the first lens element to an image-side surface of the fourth lens element is InTL, half of a maximum viewable angle of the optical image capturing system is denoted by HAF; the optical image capturing system has a maximum image height HOI on the first image plane perpendicular to the optical axis; a maximum effective diameter of the image-side surface of the fourth lens element is denoted by PhiA4; a distance on the optical axis between the first image plane and the second image plane is denoted by FS; thicknesses of the first to fourth lens elements at height of ½ HEP paralleling the optical axis are respectively ETP1, ETP2, ETP3 and ETP4; a sum of ETP1 to ETP4 described above is SETP; central thicknesses of the first to fourth lens elements on the optical axis are respectively TP1, TP2, TP3 and TP4; a sum of TP1 to TP4 described above is STP; conditions as follows are satisfied: 1≦f/HEP≦10, 0 deg<HAF≦150 deg, 0.5≦SETP/STP<1, 0<PhiA4/InTL≦5, and |FS|≦30 μm.
 2. The optical image capturing system of claim 1, wherein a wavelength of the infrared light ranges from 700 nm to 1300 nm, and the first spatial frequency is denoted by SP1, which satisfies the following condition: SP1≦440 cycles/mm.
 3. The optical image capturing system of claim 1, wherein a horizontal distance paralleling the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to the first image plane is ETL; a horizontal distance paralleling the optical axis from the coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP is EIN; conditions as follows are satisfied: 0.2≦EIN/ETL<1.
 4. The optical image capturing system of claim 1, wherein an image-side surface of the second lens element and an image-side surface of the third lens element on the optical axis are convex surfaces.
 5. The optical image capturing system of claim 1, wherein half of a vertical maximum viewable angle of the optical image capturing system is denoted by VHAF, and the following conditions are satisfied: VHAF≧10 deg, 0<PhiA4/HEP≦4.0, and 0<PhiA4/2HOI≦2.0.
 6. The optical image capturing system of claim 1, wherein the optical image capturing system satisfies the following condition: HOS/HOI≧1.2.
 7. The optical image capturing system of claim 1, wherein a horizontal distance paralleling the optical axis from the coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP is EIN; and condition as follow is satisfied: 0.3≦SETP/EIN≦1.
 8. The optical image capturing system of claim 1, wherein a horizontal distance paralleling the optical axis from a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP to the first image plane is EBL, a horizontal distance paralleling the optical axis from an axial point on the image-side surface of the fourth lens element to the first image plane is BL, and conditions as follows are satisfied: 0.1≦EBL/BL≦1.5.
 9. The optical image capturing system of claim 1, further comprising an aperture stop; wherein a distance from the aperture stop to the first image plane on the optical axis is InS, which satisfies condition as follows: 0.2≦InS/HOS≦1.1.
 10. An optical image capturing system, from an object side to an image side, comprising: a first lens element with positive refractive power; a second lens element with refractive power, an image-side surface thereof on the optical axis being a convex surface; a third lens element with refractive power, an image-side surface thereof on the optical axis being a convex surface; a fourth lens element with refractive power; a first image plane, which is an image plane specifically for visible light and perpendicular to an optical axis; a through-focus modulation transfer rate (value of MTF) at a first spatial frequency having a maximum value at central field of view of the first image plane, and the first spatial frequency being 220 cycles/mm; a second image plane, which is an image plane specifically for infrared light and perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency having a maximum value at central of field of view of the second image plane, and the first spatial frequency being 220 cycles/mm; and a first lens positioning element comprising a lens base, wherein the lens base is hollow and opaque, and the lens base is disposed with a barrel portion and a base portion that are interconnected; the barrel portion is configured to accommodate the first to fourth lens elements, and the base portion is between the fourth lens element and the first image plane; an outer perimeter of the base portion is longer than an outer perimeter of the barrel portion; a shortest side length of the base portion, which is measured on a plane perpendicular to the optical axis, has a maximum value denoted by PhiD; the optical image capturing system comprises four lens elements with refractive powers; at least one of the second to fourth lens elements has positive refractive power; focal lengths of the four lens elements are respectively f1, f2, f3 and f4; a focal length of the optical image capturing system is f; an entrance pupil diameter of the optical image capturing system is HEP; a distance on an optical axis from an object-side surface of the first lens element to the first image plane is HOS, a distance on the optical axis from the object-side surface of the first lens element to an image-side surface of the fourth lens element is InTL, half of a maximum viewable angle of the optical image capturing system is denoted by HAF; the optical image capturing system has a maximum image height HOI on the first image plane perpendicular to the optical axis; a maximum effective diameter of the image-side surface of the fourth lens element is denoted by PhiA4; a horizontal distance paralleling the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to the first image plane is ETL; a horizontal distance paralleling the optical axis from the coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP is EIN; a distance on the optical axis between the first image plane and the second image plane is denoted by FS; conditions as follows are satisfied: 1≦f/HEP≦10, 0 deg<HAF≦150 deg, 0.2≦EIN/ETL<1, 0 mm<PhiD≦10 mm, and |FS|≦30 μm.
 11. The optical image capturing system of claim 10, wherein modulation transfer rates of visible light at spatial frequency of 110 cycles/mm at positions of the optical axis, 0.3 HOT and 0.7 HOT on the first image plane are respectively denoted by MTFQ0, MTFQ3 and MTFQ7, and conditions as follows are satisfied: MTFQ0≧0.2, MTFQ3≧0.01, and MTFQ7≧0.01.
 12. The optical image capturing system of claim 10, wherein half of a vertical maximum viewable angle of the optical image capturing system is denoted by VHAF, and the following conditions are satisfied: VHAF≧20 deg, 0<PhiA4/HEP≦4.0, 0<PhiA4/2HOI≦2.0, and 0 mm<PhiA4≦5 mm.
 13. The optical image capturing system of claim 10, wherein the optical image capturing system satisfies the following condition: HOS/HOI≧1.4.
 14. The optical image capturing system of claim 10, wherein a horizontal distance paralleling the optical axis from a coordinate point on an image-side surface of the third lens element at height of ½ HEP to a coordinate point on an object-side surface of the fourth lens element at height of ½ HEP is ED34; a distance between the third lens element and the fourth lens element on the optical axis is IN34 and condition as follows is satisfied: 0<ED34/IN34≦50.
 15. The optical image capturing system of claim 10, wherein a horizontal distance paralleling the optical axis from a coordinate point on an image-side surface of the first lens element at height of ½ HEP to a coordinate point on an object-side surface of the second lens element at height of ½ HEP is ED12; a distance between the first lens element and the second lens element on the optical axis is IN12 and condition as follows is satisfied: 0<ED12/IN12≦35.
 16. The optical image capturing system of claim 10, wherein a thickness of the second lens element at height of ½ HEP paralleling the optical axis is ETP2, a central thickness of the second lens element on the optical axis is TP2, which satisfies condition as follows: 0.1≦ETP2/TP2≦5.
 17. The optical image capturing system of claim 10, wherein a thickness of the third lens element at height of ½ HEP paralleling the optical axis is ETP3, a central thickness of the third lens element on the optical axis is TP3, which satisfies condition as follows: 0.1≦ETP3/TP35≦5.
 18. The optical image capturing system of claim 10, wherein a thickness of the fourth lens element at height of ½ HEP paralleling the optical axis is ETP4, a central thickness of the fourth lens element on the optical axis is TP4, which satisfies condition as follows: 0.1≦ETP4/TP4≦5.
 19. The optical image capturing system of claim 10, wherein at least one lens element among the first lens element, the second lens element, the third lens element and the fourth lens element is a filter element of light with wavelength of less than 500 nm.
 20. An optical image capturing system, from an object side to an image side, comprising: a first lens element with positive refractive power; a second lens element with refractive power, an image-side surface thereof on the optical axis being a convex surface; a third lens element with refractive power, an image-side surface thereof on the optical axis being a convex surface; a fourth lens element with refractive power; a first average image plane, which is an image plane specifically for visible light and perpendicular to an optical axis; the first average image plane being installed at the average position of the defocusing positions, where through-focus modulation transfer rates (values of MTF) of the visible light at central field of view, 0.3 field of view, and 0.7 field of view are at their respective maximum at a first spatial frequency; the first spatial frequency being 220 cycles/mm; a second average image plane, which is an image plane specifically for infrared light and perpendicular to the optical axis; the second average image plane being installed at the average position of the defocusing positions, where through-focus modulation transfer rates of the infrared light (values of MTF) at central field of view, 0.3 field of view, and 0.7 field of view are at their respective maximum at the first spatial frequency; the first spatial frequency being 220 cycles/mm; and a first lens positioning element comprising a lens base; and a second lens positioning element accommodated in the lens base, wherein the lens base is hollow and opaque, and the lens base is disposed with a barrel portion and a base portion that are interconnected; the barrel portion is configured to accommodate the first to fourth lens elements, and the base portion is between the fourth lens element and the first average image plane; an outer perimeter of the base portion is longer than an outer perimeter of the barrel portion; a shortest side length of the base portion, which is measured on a plane perpendicular to the optical axis, has a maximum value denoted by PhiD; the second lens positioning element comprises a positioning portion and a connecting portion; the positioning portion is hollow and comes into direct contact with any lens elements to accommodate those lens elements, such that those lens elements are aligned along the optical axis; the connecting portion is disposed at an outer side of the positioning portion and comes into direct contact with an inner perimeter of the barrel portion; a maximum outer diameter of the connecting portion, which is measured on a plane perpendicular to the optical axis, is denoted by PhiC; the optical image capturing system comprises four lens elements with refractive power; at least one of the third to fourth lens elements has positive refractive power; focal lengths of the first lens element to the fourth lens elements are respectively f1, f2, f3 and f4; a focal length of the optical image capturing system is f; an entrance pupil diameter of the optical image capturing system is HEP; a distance on the optical axis from an object-side surface of the first lens element to the first average image plane is HOS, a distance on the optical axis from the object-side surface of the first lens element to an image-side surface of the fourth lens element is InTL, half of a maximum viewable angle of the optical image capturing system is denoted by HAF; the optical image capturing system has a maximum image height HOI on the first average image plane perpendicular to the optical axis; a maximum effective diameter of the image-side surface of the fourth lens element is denoted by PhiA4; a horizontal distance paralleling the optical axis from a coordinate point on the object-side surface of the first lens element at height of ½ HEP to the first average image plane is ETL; a horizontal distance paralleling the optical axis from the coordinate point on the object-side surface of the first lens element at height of ½ HEP to a coordinate point on the image-side surface of the fourth lens element at height of ½ HEP is EIN; a distance on the optical axis between the first average image plane and the second average image plane is denoted by AFS; half of a vertical maximum viewable angle of the optical image capturing system is denoted by VHAF, conditions as follows are satisfied: 1≦f/HEP≦10, 0 deg<HAF≦150 deg, |AFS|≦30 μm, VHAF≧20 deg, 0<PhiA4/InTL≦5, PhiC<PhiD, 0 mm<PhiD≦5 mm, and 0.2≦EIN/ETL<1.
 21. The optical image capturing system of claim 20, wherein thicknesses of the first to fourth lens elements at height of ½ HEP paralleling the optical axis are respectively ETP1, ETP2, ETP3 and ETP4; a sum of ETP1 to ETP4 described above is SETP; the following condition is satisfied: 0.3≦SETP/EIN<1.
 22. The optical image capturing system of claim 20, wherein the optical image capturing system satisfies the following condition: HOS/HOI≧1.6.
 23. The optical image capturing system of claim 20, wherein a linear magnification of an image formed by the optical image capturing system on the second average image plane is LM, which satisfies the following condition: LM≧0.0003.
 24. The optical image capturing system of claim 20, further comprising an aperture stop and an image sensing device; wherein the image sensing device is disposed on the first average image plane and comprises at least 100 thousand pixels, a distance on the optical axis from the aperture stop to the first average image plane is InS; condition as follows is satisfied: 0.2≦InS/HOS≦1.1.
 25. The optical image capturing system of claim 20, further comprising an aperture stop, an image sensing device, and a driving module, wherein the image sensing device is disposed on the first average image plane and comprises at least 100 thousand pixels, a distance from the aperture stop to the first average image plane is InS, and the driving module couples with the four lens elements and enables movements of those lens elements; conditions as follows are satisfied: 0.2≦InS/HOS≦1.1. 